Patent Publication Number: US-2009218481-A1

Title: High-Speed Molecular Analyzer System and Method

Description:
BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The present invention relates in general to an improved method, apparatus and system for analyzing molecules. More specifically, the invention relates to an improved method, apparatus and system for determining characteristics or properties of molecules isolated, for example, according to their mass. 
     2. Description of the Background 
     Advances in the understanding of molecular biology and genetics and the future promise of biotechnology have created a need for improved tools to further the research that will revolutionize the world. New information provided by projects such as the Human Genome Project has created even more demand for faster, higher throughput methods for sequencing DNA. The tremendous efforts put into sequencing in the last decade have helped other researchers begin to understand fundamental cell function. These efforts have accelerated the pace of research and discoveries and have created a growing need for improved tools for analyzing a large variety of molecules in addition to DNA. The benefits to mankind in medicine, agriculture and for the environment, as well as the economic potential that these fields promise, are driving researchers to decipher the function of individual genes, molecules and the cells that contain them. By sequencing an organisms&#39; DNA and analyzing the molecules that make up its cells, researchers are able to develop an understanding of the systems and structure that make it function. 
     DNA sequencing has become an extremely important tool in molecular biology. DNA sequencing is the process of determining the nucleotide order of a given DNA fragment, called the DNA sequence. The amount of DNA sequence that organisms have varies from species to species but in all but the simplest organisms, the amount that must be determined is enormous. The Human Genome for example, consists of more than 3 billion nucleotide or “bases.” The real benefit from genomics will not be derived from just the sequence data; it will be from an understanding of the function of the genes and the proteins that they encode. In order to determine the function and significance of different genes it is particularly helpful to compare the DNA sequence of entirely different species as well as the DNA sequence of like species. The DNA sequence varies even for organisms of the same species and it is these differences that determine the different characteristics of different individuals. By obtaining the sequence data from many different organisms and individuals and correlating the different characteristics with differences in the genes, great insight can be gained about genetic function. However, this requires very large amounts of sequencing capacity. There have been many methods and machines developed to improve the speed and throughput of DNA sequencing, however it has taken thousands of people, hundreds of machines and several years just to sequence the human genome using the current technology. This is entirely too slow and too costly to be practical to meet the future needs of genomics. 
     A variety of different sequencing approaches have been developed however currently, almost all DNA sequencing is performed using a version of the chain termination method, developed by Frederick Sanger. This technique uses sequence-specific termination of an in vitro DNA polymerase catalyzed synthesis reaction using modified nucleotide substrates. The synthesized copies of the original DNA are then separated by electrophoresis and analyzed to determine the sequence of the original DNA. 
     The tremendous amount of DNA sequence that is now available in databases such as GenBank serves as a valuable resource and strong enticement to generate more sequence. Disciplines such as functional genomics and proteomics have arisen and use this data along with other research techniques to go beyond simple genes to begin to decipher the secrets of life. The growth of research in these fields has created a need for improved methods for analyzing other molecules such as proteins, carbohydrates, RNA, lipids and other bio-molecules in addition to the need for higher throughput, less expensive DNA sequencing technology. 
     Researchers make use of numerous analytical techniques to characterize and decipher the functions of molecules from living systems. Analytical techniques such as high performance liquid chromatography, mass spectrography, nuclear magnetic resonance, electron microscopy, x-ray fluorescence analysis, x-ray crystallography, spectrographic absorption and fluorescence analysis and many others each yield different bits of information very helpful to researchers. As the amount of research increases so has the number of samples to be analyzed. Many techniques in use today are still suited mainly for low throughput analysis. 
     Much of the sequence generated for the Human Genome Project was made possible in part by processes using electrophoretic analysis. 
     Electrophoretic sorting of copies of DNA to sequence a segment having 1000 bases even in some of the fastest equipment can take up to an hour or more. Typically after each run, the gel or medium for electrophoresis must be discarded or otherwise replaced or replenished which can add even more time to the process. Electrophoresis is slow, complex, and expensive and the equipment requires regular maintenance. This method is also subject to resolution problems due to the different mobility&#39;s imparted by different fluorescent dyes. Since each different dye affects the mobility differently, the movement of the tagged molecules through the gel is not purely dependant on the size of the original DNA and will be affected by which dye has been incorporated. The equipment must be reconditioned between runs which costs time and requires additional consumables. In order to sequence a single organism in a reasonable time frame it is necessary to perform a very high volume of reads in a short period. Since electrophoresis is slow, many electrophoresis machines must be purchased making the sequencing process very expensive (if not impractical for some projects) in both capital costs as well as maintenance costs. Electrophoresis is not suited to satisfy the needs for significantly higher throughput. 
     Another approach to sequencing DNA involves the use of mass spectrometers. This method uses the mass spectrometer to determine the sequence from mass measurements made on copies of the original sequence or on probe molecules. Mass spectrometry is also used to analyze atomic composition and in the identification and quantification of various molecular species in a sample. Mass spectrometry is growing in importance in molecular biology and is particularly important for use in protein analysis. 
     Mass spectrometry is also a tool of choice for analyzing bio-molecules. Many different approaches have been taken to improve detectors to help increase their utility. A common limitation that time of flight mass spectrometers have is the resolution that they are able to achieve when trying to simultaneously measure a broad range of molecules with large differences in mass. For example, when sequencing DNA using mass spectrometry, it is difficult to resolve the mass differences necessary to accurately identify the base for a given position when trying to sequence a molecule with more than about 50 bases. 
     To achieve good resolution in mass spectrometry, it is desirable that molecules of like size be tightly clumped with minimal overlap to provide discrete arrival times at the detector. Poor separation of different molecule species results in less resolution. Since the velocity of the molecule is proportional to its mass, small relative differences in mass result in small differences in velocity. One source of error is due to initial velocities that the molecules have before acceleration. These differences in velocity provide error that is difficult to distinguish from velocity differences caused by differences in mass. This means that measurements on large molecules such as oligonucleotides from a sequencing reaction that differ by only the slight difference in molecular mass between A, C, G or T become more difficult to resolve as the size of the entire molecule increases. This method has typically been limited to sequencing shorter lengths of nucleic acid due to the accuracy and resolution required for larger molecules. Additionally to improve resolution four separate reactions have been run for each of the A, C, G and T and then sequenced separately and re-assembled. 
     The detectors in time of flight mass spectrometers are typically less sensitive to larger molecules with low energies. If a mixture of nucleic acid sequence fragments is analyzed that contains a large number of fragments of different lengths, the small molecules will be detected, but the larger molecules must be accelerated at the end of the drift region in order to provide enough impact to provide a signal on the detector. This introduces additional complexity and source for error. This is another aspect that contributes to the difficulty that mass spectrometers have in providing good resolution when analyzing a group of molecules with a large range of mass values. Since many molecules of interest in molecular biology are large this is a limitation that would be helpful to overcome. 
     The detectors also have a limited life that depends on the number of molecules that strike them. This means that regular maintenance and replacement is usually required to keep them accurate, this increases cost and down time. This is problematic for a machine that is to be used for high-volume sequencing since by the very nature of the process, very large quantities of molecules must be processed. 
     Background noise is also a problem with many devices. Collisions of stray molecules with the detector cause noise that reduces sensitivity. For example, molecules that are either from the desorption matrix (in the case of MALDI-TOF) or become fragmented during acceleration and or drift can produce a signal that is not discernable from the actual molecules being measured. 
     Several examples of patents and publications which disclose various DNA sequencing methods and devices or attempts to solve some of the above problems are set forth as follows. Each of the following patents and publications is incorporated by reference herein. 
     U.S. Pat. No. 5,171,534 to Smith et al., entitled “Automated DNA sequencing technique,” sets forth a system for the electrophoretic analysis of DNA fragments produced in DNA sequencing operations comprising: a source of chromophore or fluorescent tagged DNA fragments; a zone for contacting an electrophoresis gel; means for introducing said tagged DNA fragments to said zone; and photometric means for monitoring said tagged DNA fragments as they move through said gel. 
     U.S. Pat. No. 6,847,035B2 to Sharma, entitled “Devices and methods for the detection of particles,” discloses devices and methods for determining the masses of particles by measuring the time between a first event such as a sample being ionized, (or a beam of electromagnetic radiation being scattered by a particle and electromagnetic radiation scattered by said particle being detected by a detection means), and a second event in which a beam of electromagnetic radiation is scattered by a particle from said ionized sample and electromagnetic radiation from said beam scattered by said particle is detected by a detection means. 
     U.S. Pat. No. 6,995,841B2 to Scott et al., entitled “Pulsed-multiline excitation for color-blind fluorescence detection,” discloses a technology called Pulse-Multiline Excitation or PME. This technology provides a novel approach to fluorescence detection with application for high-throughput identification of informative SNPs, which could lead to more accurate diagnosis of inherited disease, better prognosis of risk susceptibilities, or identification of sporadic mutations. The PME technology has two main advantages that significantly increase fluorescence sensitivity: (1) optimal excitation of all fluorophores in the genomic assay and (2) “color-blind” detection, which collects considerably more light than standard wavelength resolved detection. Successful implementation of the PME technology will have broad application for routine usage in clinical diagnostics, forensics, and general sequencing methodologies and will have the capability, flexibility, and portability of targeted sequence variation assays for a large majority of the population. 
     U.S. Publication No. 2004/0057050 to Beck et al., entitled “Analysis systems detecting particle size and fluorescence,” sets forth particle analyzing systems with fluorescence detection, primarily in connection with particle sizing based on scattered light intensity or time-of-flight measurement. In one system, emission of fluorescence is used as a threshold for selecting particles for further analysis, e.g. mass spectrometry. In another embodiment, laser beams arranged sequentially along an aerosol path are selectively switched on and off, to increase the useful life of components, and diminish the potential for interference among several signals. Other embodiments advantageously employ color discrimination in aerodynamic particle sizing, single detectors positioned to sense both scattered and emitted fluorescent radiation, and laser beam amplitude or gain control to enhance the range of fluorescence detection. 
     U.S. Pat. No. 6,806,464 to Stowers et al., entitled “Method and device for detecting and identifying bio-aerosol particles in the air,” discloses a method for detecting and identifying bioaerosol particles in the air, the bioaerosol particles in a particle stream are selected in an ATOFMS (aerosol time-of-flight mass spectrometer) by means of fluorescence techniques, and only the selected bioaerosol particles are ionized, for instance on the basis of MALDI (matrix-assisted laser desorption/ionization), after which the resulting ions are detected and the bioaerosol particles are identified. The selection of bioaerosol particles takes place by means of laser radiation, generated by a first laser device, of a wavelength which in specific substances in bioaerosol particles effects a fluorescence, after which by means of a fluorescence detector the bioaerosol particles are selected and a second laser device is triggered to emit light of a wavelength which effects the ionization of the bioaerosol particles selected only by the fluorescence detector. 
     U.S. Pat. No. 5,003,059 to Brennan, entitled “Determining DNA sequences by mass spectrometry,” relates to the methods, apparatus, reagents and mixtures of reagents for sequencing natural or recombinant DNA and other polynucleotides. In particular, this invention relates to a method for sequencing polynucleotides based on mass spectrometry to determine which of the four bases (adenine, guanine, cytosine or thymine) is a component of the terminal nucleotide. In particular, the present invention relates to identifying the individual nucleotides by the mass of stable nuclide markers contained within either the dideoxynucleotides, the DNA primer, or the deoxynucleotide added to the primer. This invention is particularly useful in identifying specific DNA sequences in very small quantities in biological products produced by fermentation or other genetic engineering techniques. The invention is therefore useful in evaluating safety and other health concerns related to the presence of DNA in products resulting from genetic engineering techniques. 
     U.S. Pat. No. 5,643,798 to Beavis, et al., entitled “Instrument and method for the sequencing of genome,” is directed to improved techniques for DNA sequencing, and particularly for sequencing of the entire human genome. Different base-specific reactions are utilized to use different sets of DNA fragments from a piece of DNA of unknown sequence. Each of the different sets of DNA fragments has a common origin and terminates at a particular base along the unknown sequence. The molecular weight of the DNA fragments in each of the different sets is detected by a matrix assisted laser absorption mass spectrometer to determine the sequence of the different bases in the DNA. The methods and apparatus of the present invention provide a relatively simple and low cost technique which may be automated to sequence thousands of gene bases per hour, and eliminates the tedious and time consuming gel electrophoresis separation technique conventionally used to determine the masses of DNA fragments. 
     U.S. Pat. No. 5,691,141 to Koster, entitled “DNA sequencing by mass spectrometry,” sets forth a new method to sequence DNA. The improvements over the existing DNA sequencing technologies are high speed, high throughput, no electrophoresis and gel reading artifacts due to the complete absence of an electrophoretic step, and no costly reagents involving various substitutions with stable isotopes. The invention utilizes the Sanger sequencing strategy and assembles the sequence information by analysis of the nested fragments obtained by base-specific chain termination via their different molecular masses using mass spectrometry, as for example, MALDI or ES mass spectrometry. A further increase in throughput can be obtained by introducing mass-modifications in the oligonucleotide primer, chain-terminating nucleoside triphosphates and/or in the chain-elongating nucleoside triphosphates, as well as using integrated tag sequences which allow multiplexing by hybridization of tag specific probes with mass differentiated molecular weights. 
     U.S. Pat. Nos. 6,541,765B1 and 6,281,493B1 to Vestal, both entitled “Time-of-flight mass spectrometry analysis of biomolecules,” are directed to a time-of-flight mass spectrometer for measuring the mass-to-charge ratio of a sample molecule. The spectrometer provides independent control of the electric field experienced by the sample before and during ion extraction. Methods of mass spectrometry utilizing the principles of this invention reduce matrix background, induce fast fragmentation, and control the transfer of energy prior to ion extraction. 
     U.S. Pat. No. 5,998,215 to Prather et al., entitled “Portable analyzer for determining size and chemical composition of an aerosol,” discloses a portable analyzer for determining the size and chemical composition of particles suspended in an aerosol. The aerosol is accelerated through a nozzle and skimmers, to produce a well-defined beam of particles, the speed of which is inversely related to the particle size. A dual-beam laser system positioned along the beam path detects light scattered from each particle, to determine the particle&#39;s velocity and thus its aerodynamic size. The laser system also triggers a laser to produce a beam that irradiates the particle, to desorb it into its constituent molecules. The particle is desorbed in a source region of a bipolar, time-of-flight mass spectrometer, which provides a mass-to-charge spectrum of the desorbed molecule, thereby chemically characterizing the material of the particle. Several structural features provide sufficient ruggedness to allow the analyzer to be easily used in the field with minimum calibration and maintenance. 
     U.S. Pat. No. 5,681,752 to Prather et al., entitled “Method and apparatus for determining the size and chemical composition of aerosol particles,” sets forth an improved mass spectrometer apparatus, and related method, that characterizes aerosol particles, in real time, according not only to their chemical composition, but also to their size. This added information can be of critical importance when evaluating risks associated with aerosol particles of particular chemical composition. The apparatus achieves this beneficial result in a reliable fashion by first detecting the presence and size of individual aerosol particles moving along a predetermined particle path and by then directing a pulse of high-intensity light at the particle, to desorb and ionize the particle, for analysis of its chemical composition. 
     U.S. Pat. No. 5,654,545 to Holle et al., entitled “Mass resolution in time-of-flight mass spectrometers with reflectors,” discloses a method for the high resolution analysis of analyte ions in a time-of-flight mass spectrometer. The method consists of the generation of an intermediate time-focus plane for ions of a certain mass at a location between an ion source and an ion reflector, and then using the ion reflector to temporally focus the ions of equal mass and differing velocities which pass this plane at the same time onto a detector. For time-of-flight mass spectrometers with an ion selector, the ion selector is particularly favorable location for this intermediate plane with time focus; and with a collision cell for the collision fragmentation of the ions, the collision cell is a particularly favorable location. 
     Various articles and publications include the following: 
     Mark T. Roskey, Peter Juhasz, Igor P. Smirnov, Edward J. Takach, Stephen A. Martin and Lawrence A. Haff (1996). DNA sequencing by delayed extraction-matrix-assisted laser desorption/ionization time of flight mass spectrometry. Proc. Natl. Acad. Sci. USA. Vol. 93, pp. 4724-4729, May 1996. Biochemistry. PerSeptive Biosystems, 500 Old Connecticut Path, Framingham, Mass. 01701. Communicated by Klaus Biemann, Massachusetts Institute of Technology, Cambridge, Mass., Jan. 11, 1996 (received for review Nov. 10, 1995). http://www.pubmedcentral.nih.gov/picrender.fcgi?artid=39346&amp;blobtype=pdf 
     Finn Kirpekar*, Eckhard Nordhoff, Leif K. Larsen, Karsten Kristiansen, Peter Roepstorff, Franz Hillenkamp (1998). DNA sequence analysis by MALDI mass spectrometry. Department of Molecular Biology, Odense University, Campusvej 55, DK-5230 Odense M, Denmark and  1 Institute for Medical Physics and Biophysics, University of Münster, Robert-Koch-Strasse 31, D-48149 Münster, Germany. Received Mar. 10, 1998; Revised and Accepted Apr. 16, 1998. http://nar.oxfordjournals.org/cgi/content/abstract/26/11/2554
     N. I. Taranenko, S. L. Allman, V. V. Golovlev, N. V. Taranenkol, N. R. Isola and C. H. Chen* (1998). Sequencing DNA using mass spectrometry for ladder detection. 2488-2490 Nucleic Acids Research, 1998, Vol. 26, No. 10. Life Science Division, Oak Ridge National Laboratory, Oak Ridge, Tenn. 37831-6378, USA and 1 Yale University Medical Center, New Haven, Conn., USA. Received Dec. 3, 1997; Revised and Accepted Mar. 23, 1998. http://www.pubmedcentral.nih.gov/picrender.fcgi?artid=147544&amp;blobtype=pdf   

     Eckhard Nordhoff, a  Christine Luebbert, Gabriela Thiele, Volker Heiser, and Hans Lehrach (2000). Rapid determination of short DNA sequences by the use of MALDI-MS. Nucleic Acids Res. 2000 Oct. 15; 28(20): e86. Max Planck Institute for Molecular Genetics, Ihnestrasse 73, 14195 Berlin, Germany. To whom correspondence should be addressed. Tel: +49 30 8413 1542; Fax: +49 30 8413 1139; Email: nordhoff@molgen.mpg.de. Received Aug. 21, 2000; Accepted Aug. 22, 2000. http://www.pubmedcentral.nih.gov/articlerender.fcgi?artid=110802
     Annette Kaetzke and Klaus Eschrich (2002). Simultaneous determination of different DNA sequences by mass spectrometric evaluation of Sanger sequencing reactions. Nucleic Acids Research, 2002, Vol. 30, No. 21 e117. Institute of Biochemistry, Medical Faculty, University of Leipzig, Liebigstrasse 16, D-04103 Leipzig, Germany. *To whom correspondence should be addressed. Tel: +49 341 9722105; Fax: +49 341 9739371; Email: eschrich@uni-leipzig.de http://nar.oxfordjournals.org/cgi/content/abstract/30/21/e117   

     While the mass spectrometer can provide fast analysis of molecules, numerous practical limitations prevent it from being the high throughput tool that is needed. A sequencing method that can provide the speed of mass spectrometry and the convenience of one sequencing reaction for all bases as well as good read lengths is clearly needed. Therefore, there is a need to determine the sequence of nucleic acids and analyze other molecules and collections of molecules in a much faster and more economical way. Additionally, a high throughput instrument for analyzing molecules such as bio-molecules is needed and would be particularly helpful in analyzing biological systems. Whatever the precise merits features and advantages of the above cited references, none of them achieves or fulfills the purpose of the present invention as set forth below. 
     Those of skill in the art will appreciate the present invention which addresses the above needs and other significant needs the solution to which are discussed hereinafter. 
     SUMMARY OF THE INVENTION 
     The present invention contemplates a method and apparatus for analyzing at least one molecule. An aspect of the invention is Isolating at least one molecule wherein the isolating depends substantially on the mass of the at least one molecule; subsequently Interacting the at least one molecule with a radiant signal inducer; and detecting a signal resulting from the interacting of the at least one molecule and the radiant signal inducer. 
     Analyzing includes but is not limited to determining: the atomic composition of one or more molecules; the mass of one or more molecules; at least one subunit of at least one molecule comprising two or more subunits; and the concentration of one or more molecules in a sample. Analyzing also may include but is not limited to nucleic acid sequencing; DNA sequencing; single nucleotide polymorphism (SNP) analysis; and protein sequencing. 
     The at least one molecule includes but is not limited to organic molecules as well as inorganic molecules. Organic molecules include but are not limited to bio-molecules. Inorganic molecules include but are not limited to inorganic monomers and inorganic polymers. Bio-molecules include but are not limited to: small molecules; organic monomers; organic polymers and macromolecules. Small molecules include but are not limited to: lipids, phospholipids, glycolipids, sterols; vitamins; hormones, neurotransmitters, carbohydrates, sugars and disaccharides. Monomers include but are not limited to amino acids, nucleotides, phosphates and monosaccharides. Organic polymers include but are not limited to nucleic acids, peptides, oligosaccharides and polysaccharides. Macromolecules include but are not limited to prions. Nucleic acids include but are not limited to DNA, RNA and oligonucleotides. Peptides include but are not limited to oligopeptides, polypeptides, proteins and antibodies. 
     Other embodiments of the invention are configured to analyze molecules such as: at least one fragment molecule wherein the fragment has been prepared by using the at least one molecule as a template. The at least one fragment molecule may also have a known subunit in a known position on the fragment. Additionally, molecules to be analyzed may comprise a tag that is capable of producing a signal when interacted with a signal inducer such as but not limited to a fluorophore. One embodiment of the invention analyzes a molecule comprising a subunit comprising a fluorescent tag in a known position wherein the tag is characteristic of the subunit comprises it. 
     The isolating depending substantially on the mass of the at least one molecule may have numerous embodiments including but not limited to the following: one embodiment comprises ionizing and accelerating the at least one molecule to be analyzed and allowing it to drift a sufficient distance to allow isolation dependent upon its mass; one embodiment of the invention comprises a time of flight (TOF) mass analyzer; one embodiment of the invention comprises a quadrupole mass analyzer; another embodiment comprises a magnetic-sector mass analyzer; another embodiment comprises a quadrupole ion trap mass analyzer and a further embodiment comprises a Fourier transform ion cyclotron resonance mass analyzer. 
     In one embodiment of the invention the radiant signal inducer comprises electromagnetic radiation. Another embodiment of the invention comprises particle radiation. Examples of electromagnetic radiation suitable for various embodiments of the invention include: radio frequency radiation, microwave radiation, infrared radiation, visible light, ultraviolet light, x-ray radiation and gamma ray radiation. Examples of particle radiation suitable for various embodiments of the invention include: protons neutrons, electrons, positrons, alpha particles and molecules. These types of radiation can be used separately or in combination 
     One example embodiment comprises a laser as a source of a radiant signal inducer. The laser may independently comprise a diode laser, a semiconductor laser, a gas laser, such as an argon ion, krypton, or helium-neon laser, a diode laser, a solid-state laser such as a Neodymium laser which will include an ion-gain medium, such as YAG and yttrium vanadate (YVO 4 ), or a diode pumped solid state laser. Other devices, which produce light at one or more discrete excitation wavelengths, may also be used as a source of radiant signal inducer such as a flash lamp. One example embodiment the source of radiant signal inducer comprises a xenon flash lamp. Another example embodiment the source of a radiant signal inducer comprises an x-ray tube. 
     In one example embodiment the source of a radiant signal inducer comprises a source of particles. Examples of sources of particles include an electron gun and radioisotopes. 
     An aspect of the present invention includes interacting at least one molecule with a radiant signal inducer after being isolated depending substantially upon the mass of the at least one molecule. One example embodiment comprises a time of flight mass analyzer and a laser beam directed to intersect the flight path of the at least one molecule through the TOF mass analyzer such that when the at least one molecule passes through the TOF mass analyzer it interacts with the laser beam. Another example embodiment comprises a quadrupole ion cyclotron mass analyzer and an x-ray tube disposed generally at the exit of the quadrupole ion cyclotron mass analyzer such that when the at least one molecule exits the mass analyzer it passes through the x-ray radiation emitted from the x-ray tube and thereby interacts with the x-ray radiation and produces a signal characteristic of a property of the at least one molecule. 
     In one example embodiment the radiant signal inducer radiates in substantially parallel paths from at least one source. In another example embodiment the radiant signal inducer radiates in substantially non-parallel paths from at least one source. 
     The signal inducer may be emitted continuously from at least one source or be emitted in one or more pulses from at least one source. The pulsed emission may comprise control circuitry to control the emission of the one or more pulses. 
     The signal produced as a result of the interaction of the radiant signal inducer may, comprise any form of electromagnetic radiation or particle radiation or combinations of the same. The signal produced can be the result of luminescence such as fluorescence resulting from the interaction. Interaction of the radiant signal inducer and the at least one molecule can be detected by: detecting absorption of the radiant signal inducer by the at least one molecule or by detecting emission of a particle or electromagnetic radiation or by detecting scattering of the radiant signal inducer or by detecting reflection of the radiant signal inducer or by detecting a combination of two or more of these phenomena. 
     The detector may comprise a charged couple device, a photomultiplier tube, a silicon avalanche photodiode, a silicon PIN detector, a wavelength dispersive spectrometer or an energy dispersive spectrometer. It may also comprise filters to selectively pass or block electromagnetic radiation or particles depending upon the wavelength of the electromagnetic radiation or the energy of the signal to be detected or the type of particle. 
     The present invention may further comprise data processing apparatus for processing of the signals detected. 
     In one example embodiment, a method for analyzing at least one molecule is provided. The method includes at least: providing at least one molecule; isolating the at least one molecule; causing the at least one molecule to emit a signal; and detecting the signal. 
     Another example embodiment of an apparatus includes a novel device for the analysis of nucleic acid fragments including at least: a source of chromophore or fluorophore tagged nucleic acid fragments, the chromophore of fluorophore being distinguishable by the spectral characteristics; means for vaporization and acceleration of said nucleic acid fragments; means for introducing the tagged nucleic acid fragments to the vaporization and acceleration means; a drift region; said vaporization and acceleration means being located at one end of said drift region and directed so as to propel said nucleic acid fragments through said drift region; detecting means located at the end of said drift region generally opposite said accelerating and vaporization means; said detecting means comprises means for inducing emission from the tagged nucleic acid fragments and means for detecting emissions from said tagged nucleic acid fragments and distinguishing said tagged nucleic acid fragments. 
     In another example embodiment of the apparatus, the apparatus includes at least vaporization and ionization means comprising electro-spray ionization. 
     In another example embodiment of the apparatus, the apparatus includes at least a vaporization and ionization means comprising matrix assisted laser desorption ionization. 
     In another example embodiment of the apparatus, the apparatus includes at least a source of illumination comprising a laser. 
     In another example embodiment of the apparatus, the apparatus includes at least means for detecting emissions comprising a prism and one or more photo detectors located at positions corresponding to unique spectral positions. 
     Another example embodiment of a method includes a method of determining the sequence of nucleic acids comprising the following steps: introduction of chromophore of fluorophore tagged nucleic acid fragments, said chromophore of fluorophore being distinguishable by its spectral characteristics; vaporization of said nucleic acid fragments; acceleration of said nucleic acid fragments; stimulation of said nucleic acid fragments by external means so as to induce emissions from said tag; and detection of said emissions. 
     Another example embodiment of an apparatus includes a device for the determination of the sequence of a nucleic acid sample comprising: a generally tubular chamber; said chamber being evacuated sufficiently to prevent degradation of said sample during analysis; means for electrospray ionization of said sample; an accelerating grid adjacent the injector; an un-obstructed section of sufficient length to allow separation of said sample after acceleration by said accelerating grid; a laser directed to intersect the path of flight of said sample, positioned at the end of said un-obstructed section, opposite said accelerating grid; a photo-detector located sufficiently close to said intersection of said illumination source and said path of flight of said sample. 
     Another example embodiment comprises a photo-detector located sufficiently close to said intersection of said illumination source and said path of flight of said sample. 
     Another example embodiment comprises an unobstructed section of sufficient length to allow separation of said sample after acceleration by said accelerating grid. 
     Another example embodiment comprises a source of illumination directed to intersect said path of flight of said nucleic acid fragments, positioned at the end of said tubular chamber, opposite said vaporization and acceleration means. 
     Another example embodiment comprises a chamber being evacuated sufficiently to prevent degradation of said nucleic acid fragments during analysis. 
     Another example embodiment comprises at one end of said chamber, means for vaporization and acceleration of said nucleic acid fragments along a path of flight generally in the direction of the axis of said tubular chamber. 
     Another example embodiment provides a method for analyzing at least one molecule Comprising: Providing item to be analyzed; isolating the item to be analyzed; causing the item to be analyzed to emit a signal. 
     Another example embodiment provides a method for analyzing at least one molecule comprising: providing at least one molecule; isolating the at least one molecule; causing the at least one molecule to emit a signal; and detecting the signal. 
     Another example embodiment provides a method for analyzing at least one molecule comprising: providing at least one molecule; causing the at least one molecule to have a non-neutral charge; separating the at least one molecule based on its mass to charge ratio; causing the at least one molecule to emit a detectable signal; detecting said signal; recording said signal. 
     Another example embodiment provides a method for determining the identity of at least one base of at least one polynucleotide comprising: providing a population of fluorescently labeled fractions; each fraction having a unique fluorescent label characteristic of the base at its end position; accelerating the population of fractions in a manner so as to impart generally the same amount of energy to each molecule; allowing the population of fractions to travel a distance sufficient to separate like fractions into differentiable groups; causing at least one of the fluorescent labels on at least one of the fractions to fluoresce; and detecting the signal emitted from the label. 
     Another example embodiment provides a method for analyzing at least one molecule comprising: providing at least one molecule; accelerating the at least one molecule; allowing the at; least one molecule to travel a distance; causing the at least one molecule to emit a detectable signal; detecting said signal; recording said signal. 
     Another example embodiment of the method includes at least sequencing a group of molecules, wherein each molecule comprises multiple sub-units of differing sub-unit types, wherein each of the molecules includes at least one tag specific to the sub-unit type, the method comprising: accelerating said molecules, separating said molecules dependant upon at least said accelerating, and radiant detecting of each of the at least one tags by the tag type of each of the at least one tags. 
     In another example embodiment of the method, the method includes at least radiant detecting comprises electromagnetic radiant detecting. 
     In another example embodiment of the method, the method includes at least radiant detecting comprising phosphorescent radiant detecting. 
     In another example embodiment of the method, the method includes at least radiant detecting comprising fluorescent radiant detecting. 
     In another example embodiment of the method, the method includes at least radiant detecting comprising thermal radiant detecting. 
     In another example embodiment of the method, the method includes at least radiant detecting comprising radioactive radiant detecting. 
     In another example embodiment of the method, the method includes at least radiant detecting comprising particle radiant detecting. 
     In another example embodiment of the method, the method includes at least radiant detecting comprising chemical-reactive radiant detecting. 
     In another example embodiment of the method, a further method includes at least radiant detecting comprising detecting the radiation of the tag with a detector. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising electromagnetic radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising phosphorescent radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising fluorescent radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising thermal radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising radioactive radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising particle radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising chemical-reactive radiant detecting. 
     In another example embodiment of the method, a further method includes at least radiant detecting comprising detecting the radiation of a detection substance upon contact with the tag. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising electromagnetic radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising phosphorescent radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising fluorescent radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising thermal radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising radioactive radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising particle radiant detecting. 
     In another example embodiment of the further method, the method includes at least radiant detecting comprising chemical-reactive radiant detecting. 
     In molecular biology and materials science there is a growing need for the identification and characterization molecules. The device of the current invention would allow the determination of various characteristics such as mass, absorbance and fluorescence signatures and possibly molecular structure. 
     An embodiment of the invention is an apparatus for determining the sequence of DNA molecules, however the invention can be applied to many analytical purposes in characterizing molecules. 
     A method for analyzing at least one molecule comprising: accelerating the at least one molecule; allowing the molecule to travel a distance; remotely detecting a signal from the molecule after traveling said distance; recording said signal from said detecting. 
     The apparatus for determining the sequence of DNA is similar to a time of flight mass spectrometer and has four basic components:
         1. A molecule accelerator that ionizes and accelerates the molecule of interest. This can be an apparatus such as an electro-spray device or a matrix assisted laser desorption ionization device.   2. A flight tube that is connected to the accelerator and provides a path for the molecules to travel after they are accelerated. This flight tube would be held at a vacuum to minimize collisions during the flight of the molecule being analyzed.   3. A detection device that comprises: a laser directed generally normal to the flight path of the molecules and located at the end of the flight tube opposite from the accelerator; 4 photon detectors such as photo-multiplier tubes located in the same plane as the laser and oriented generally normal to the laser beam; a refractor for dispersing light into its component colors and directing the light at one of each of the 4 photon detectors.   4. A data recording device that records the signals from each of the detectors.       

     The operation of the apparatus is as follows: The DNA to be analyzed is prepared in a manner typical for analysis in a 4 color capillary sequencing device. This process produces a population of molecules that range in length from a few molecules to the original length of the DNA molecule to be analyzed. During the sequencing reaction a fluorescent dye is incorporated at the end of each of these molecules. The tags fluoresce when excited by a laser and emit one of 4 colors representing the base for that end position. 
     The DNA prepared as described above is introduced into the accelerator component of the apparatus of the current embodiment of the invention. A group of these molecules are ionized and accelerated by the accelerator and directed to travel down the flight tube. 
     As a result of traveling the distance of the flight tube the molecules are fractionated by length. Since all molecules are imparted the same amount of energy by the accelerator, each molecule of a given length travels at a different velocity. The smallest molecules travel the fastest and the next smallest next fastest, etc. until the largest molecules which travel the slowest. This velocity difference causes the molecules to pass the detector at different times and thus accomplishes the fractionation. 
     As each molecule group passes the detector they are illuminated by the laser. This illumination causes the fluorescent dyes to emit light which passes through the refractor and is directed to the appropriate photo detector. 
     The data recording device records the detector signal strength and the time detected. 
     After all of the molecules have passed the detector, the data recorded then can be analyzed and the exact sequence of the original DNA molecule determined by correlating the wavelength detected and the order in which it was detected. 
     The present invention is shown as a block diagram in  FIG. 1 . The present invention comprises a sample accelerator  1 , a drift tube  2  and a detector  3 . The chamber in the drift tube  8  and the area inside the detector are maintained at high vacuum by vacuum pumps connected at ports  5  and  6 . The sample accelerator vaporizes, ionizes and accelerates the sample molecules down the drift tube along the path  7  and through the detector chamber  15 . While passing through the detector  3 , the sample ions are illuminated by the laser beam  11  causing the fluorescent dye terminator molecules incorporated into the sample molecules to emit light. The photo detector  9  then detects this light. The particular dye terminator incorporated at the end of the molecule corresponds to the original nucleotide of the molecule being sequenced. Once past the detector, the sample molecules are then cleared from the chamber mainly by the vacuum pump connected to port  6 . 
     Referring to the block diagram in  FIG. 1 , the sample molecules to be analyzed are vaporized and ionized by ionizing means  1 . The ionizing means  1  can be any device that provides a source of ionized molecules of sample without causing excessive degradation of the sample molecules. Devices that are commonly used to do this use techniques such as Matrix Assisted Laser Desorption Ionization (MALDI) and Electrospray Ionization (ES). These techniques are commonly used to provide sample ion sources for Time of Flight Mass Spectrometers and are well known. Each device has particular advantages and disadvantages but serves as means to convert the sample to be analyzed to a gaseous ionized collection of molecules. The ionizing means accelerates the sample molecules to a velocity that is proportional to their mass to charge ratio. Thus, the smaller molecules will have higher velocities than the larger molecules. The molecules exit the ionizing means  1  through exit port  14  with a velocity directed down the drift tube  2 . The dashed line  7  represents the flight path of the molecules, which travel down the drift tube past the detection point  13 . As the molecules travel the distance down the drift tube, the smaller (faster moving) molecules travel the distance faster than the larger molecules. This results in a separation of the sample such that the molecules pass the detection point in order of increasing size with smallest arriving first and largest arriving last. The chamber areas in the drift tube  7  and detector  15  are maintained at a high vacuum. The vacuum should be sufficient so as to prevent collisions between the sample and stray molecules causing excessive fragmentation and disruption of the sorting process. 
     The sample to be sequenced is injected at  1 . Very quickly after injection the sample breaks into very small droplets that evaporate and leave the individual molecules in a charged state. 
     After the sample is fully vaporized the accelerating grid  2  is turned on accelerating the molecules from the sample through the grid. After passing through the grid they travel down a drift section that is an un-obstructed section of the chamber. This section is of sufficient length to allow separation of said sample after acceleration by the accelerating grid. The molecules are accelerated to a velocity that is proportional to their mass to charge ratio. Therefore molecules of like mass (size) will be accelerated to very near the same velocity. As the molecules travel down the drift section, the fastest (smallest) molecules are the first to reach the detector section. The next smallest molecules arrive next and so on until all of the molecules from the sample have passed the detector section. 
     An object of the invention is to make large-scale sequencing of nucleic acids faster, simpler and lower in cost. Several other objects and advantages of the present invention are to provide a method and an apparatus to sequence polymeric or chain type molecules such as nucleic acids:
         a) in larger volumes in a shorter amount of time;   b) having larger molecular size with greater accuracy;   c) as a continuous process without requiring reconditioning between each run;   d) with lower maintenance requirements;   e) with a lower sequencing cost per base.       

     An example embodiment of the invention is a method and apparatus for determining the sequence polymeric or chain type molecules such as nucleic acids. This example embodiment comprises a source of chromophore or fluorophore tagged molecule fragments each being distinguishable by its spectral characteristics; a means for vaporization and acceleration of the molecule fragments; means for introducing the tagged molecule fragments to the vaporization and acceleration means; a drift region having the vaporization and acceleration means located at one end of the drift region and directed so that it propels the molecule fragments through the drift region; detecting means located at the end of the drift region generally opposite the accelerating and vaporization means. The detecting means comprises means for inducing emission from the tagged molecule fragments; means for detecting emissions from the tagged molecule fragments and distinguishing the tagged molecule fragments. 
     Sequencing of polymeric or chain type molecules such as DNA is accomplished by producing duplicate copies of varying lengths of the original sequence that are terminated with a base specific chromophore or fluorophore. Four different chromophores or fluorophores are used (one for each possible nucleotide) and each terminating molecule emits a unique emission spectrum when excited. The prepared DNA or nucleic acid is then loaded into the present invention for analysis. The nucleic acid fragments are then vaporized, ionized and accelerated by an electric field and directed down the drift region. The nucleic acid fragments are all subjected to approximately the same force in the accelerating field; however, since each fragment of a different length has a different mass, each is accelerated to a different final velocity. As the nucleic acid fragments travel through the drift region, their differences in velocity cause them to be sorted from smallest to largest, the smallest arriving first and largest last. The detector illuminates the molecules as they pass and a sensor receives the resulting emission. The detector is designed to sense characteristic emission spectrum of each tagged nucleotide allowing determination of the individual bases. The output from each sensor is then an accurate, ordered sequential representation of the bases in the original molecule under analysis. 
     This design achieves very high throughputs in contrast with electrophoresis. Electrophoresis can typically take at least an hour for the sample to pass completely by the detector compared to fractions of a second for the present invention. The present invention requires virtually no reconditioning. All that is necessary to prepare the machine to sequence another sample is for the vacuum pump to clear the molecules from the previous sample out of the vacuum chamber, which happens very quickly. 
     The present invention has advantages over mass spectrometry since the detection method depends on detection of the wavelength of the emission from the florescent tags not precise measurements of time between discrete collisions. 
     The apparatus required is relatively simple with very few parts to fail; therefore, the maintenance requirements are lower than the prior art. The machine can be made to operate automatically and there is next to no reconditioning required between runs so the labor cost per sample is lower than the prior art. 
     The content and disclosure of U.S. non-provisional patent application Ser. No. 11/244,550, filed Oct. 6, 2005 and U.S. provisional patent application No. 60/616,955, filed Oct. 7, 2004 are hereby incorporated by reference herein. 
     Other and further objects, advantages and features of the present invention will become apparent from a consideration of the following discussions and drawings describing various embodiments of the invention. 
     There has thus been outlined, rather broadly, the more important features of the invention in order that the detailed description thereof may be better understood, and in order that the present contribution to the art may be better appreciated. There are additional features of the invention that will be described hereinafter. 
     In this respect, before explaining at least one example embodiment of the invention in detail, it is to be understood that the invention is not limited in its application to the details of construction and to the arrangements of the components set forth in the following description or illustrated in the drawings. The invention is capable of other embodiments and of being practiced and carried out in various ways. Also, it is to be understood that the phraseology and terminology employed herein are for the purpose of the description and should not be regarded as limiting. 
     To the accomplishment of the above and related objects, this invention may be embodied in the form illustrated in the accompanying drawings, attention being called to the fact, however, that the drawings are illustrative only, and that changes may be made in the specific construction illustrated. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       The drawings as noted below form part of the present specification and are included to further demonstrate certain aspects of the present invention. Various other objects, features and attendant advantages of the present invention will become fully appreciated as the same becomes better understood when considered in conjunction with the accompanying drawings, in which like reference characters designate the same or similar parts throughout the several views, and wherein: 
         FIG. 1  shows a schematic diagram of a example nucleotide-sequencing device in accordance with the current invention. 
         FIG. 2  shows a symbolic representation of a hypothetical nucleic acid sequence paired with a complimentary nucleic acid copy terminated with a base specific label molecule. 
         FIG. 3  shows a symbolic representation of a vaporized group of hypothetical nucleic acid copies of different lengths; illustrating a random special orientation of the different length molecules. 
         FIG. 4  shows a symbolic representation of the same molecules in  FIG. 3  shortly after being accelerated; illustrating separation of the sizes. 
         FIG. 5  shows a symbolic representation of the same molecules in  FIG. 3  after being accelerated and traveling for sufficient time to effect significant separation by size. 
         FIG. 6  shows a schematic representation of the detector optics of an example embodiment. 
         FIG. 7  shows a symbolic representation of a group of molecules under analysis and the corresponding outputs from the detectors sensing them. 
         FIG. 8  shows a cross section of an example detector having a single photo detector. 
         FIG. 9  shows a schematic diagram of an example nucleic acid sequencing device in accordance with the present invention. 
         FIG. 10  shows a schematic diagram of an example molecular analysis device in accordance with the present invention. 
         FIG. 11  shows a schematic diagram of an example a wavelength dependent photon detector in accordance with the present invention. 
         FIG. 12  shows a schematic diagram of an example molecular detector in accordance with the present invention. 
         FIG. 13  shows a schematic diagram of an enlarged view of the region where a molecule is in a position to interact with the signal inducer pulses in accordance with the present invention. 
         FIG. 14  shows a schematic diagram of an enlarged view of the region where a molecule is in a position to interact with the signal inducer pulses in accordance with the present invention. 
         FIG. 15  shows a schematic diagram of an enlarged view of the region where a molecule is in a position to interact with the signal inducer pulses in accordance with the present invention. 
         FIG. 16  shows a schematic diagram of an enlarged view of the region where a molecule is in a position to interact with the signal inducer pulses in accordance with the present invention. 
         FIG. 17  shows a schematic diagram of an enlarged view of the region where a molecule is in a position to interact with the signal inducer pulses in accordance with the present invention. 
         FIG. 18  shows a schematic diagram of an enlarged view of the region where a molecule is in a position to interact with the signal inducer pulses in accordance with the present invention. 
         FIG. 19  shows a schematic diagram of the molecule in a position to interact with the radiant signal inducer and illustrates how the pulse time can be calculated in accordance with the present invention. 
         FIG. 20  shows a schematic diagram of an example molecular analysis device in accordance with the present invention. 
         FIG. 21  shows a schematic diagram of an example molecular analysis device in accordance with the present invention. 
         FIG. 22  shows a schematic diagram of an example molecular analysis device in accordance with the present invention. 
         FIG. 23  shows a schematic diagram of an example molecular analysis device in accordance with the present invention. 
         FIG. 24  shows a schematic diagram of an example molecular sequencing device in accordance with the present invention. 
         FIG. 25  shows a schematic diagram of a molecule with two or more subunits in accordance with the present invention. 
         FIG. 26  shows a schematic diagram of a molecule fragments in accordance with the present invention. 
         FIG. 27  shows a schematic diagram of a molecule fragments in accordance with the present invention. 
         FIG. 28  shows a schematic diagram of a molecule fragments in accordance with the present invention. 
         FIG. 29  shows a schematic diagram of time measurements recorded for fragment groups accordance with the present invention. 
         FIG. 30  shows a schematic diagram of an example molecular analysis device in accordance with the present invention. 
     
    
    
     While the present invention will be described in connection with presently preferred embodiments, it will be understood that it is not intended to limit the invention to those embodiments. On the contrary, it is intended to cover all alternatives, modifications, and equivalents included within the spirit of the invention and as defined in the appended claims. 
     DETAILED DESCRIPTION OF EXAMPLE EMBODIMENTS OF THE INVENTION 
     The present invention is a novel device and method for the high speed analysis of molecules for determining characteristics such as atomic composition; mass; sequence of subunits and the concentration of one or more molecules in a sample. The invention may also be used for nucleic acid sequencing; DNA sequencing; single nucleotide polymorphism (SNP) analysis; and protein sequencing. 
     In one example embodiment of the invention an apparatus is provided for determining the sequence of bases or nucleotides in a nucleic acid such as DNA or RNA. 
     The basic steps involved in the process include:
         a) Making copies ranging in length from 1 nucleotide to the same length as the molecule under analysis;   b) Incorporating a base specific molecule at the end of the copy that corresponds to the base of the original molecule at that position and has a dye molecule that emits a uniquely identifiable spectrum when induced by external means;   c) Vaporizing the molecules;   d) Accelerating the molecules in a way so as to impart substantially the same energy to each molecule;   e) Allowing the molecules to travel for a sufficient time after acceleration so that the molecules are able to be separated as a consequence of their differences in velocity;   f) Inducing an emission from the molecules in a localized area of the path of travel after time for separation has elapsed;   g) Detecting the emissions from the molecules.       

     A detailed description of each of the steps listed above will now be given generally in the order that they are presented. 
     In an example embodiment, nucleic acid that is to be analyzed is prepared by producing copies ranging in length from a few nucleotides up the same length as the original sample molecule. When these copies are produced care is taken so as to produce generally equivalent numbers of molecules of each given length. At the end of each molecule, a fluorescent dye is incorporated in place of the original nucleotide. Four different dyes are used in the preparation of the copies, one for each of the four possible nucleotides. Each of these dyes has unique emission spectra when induced by external means such as illumination by a light source such as a laser. 
     There are various techniques for preparing the samples to achieve the desired results mentioned above. The most common method involves the use of the enzymatic chain termination reaction. This method is widely used and well known. This technique involves the Polymerase Chain Reaction (PCR) to make copies of the original sequence. During the copying, a dideoxynucleotide with a fluorescent dye molecule attached is incorporated randomly during PCR this halts the copying of the chain at the point where it is incorporated. Sufficient PCR cycles are run so that large enough populations of base specific terminated fragments of different lengths exist to allow detection by the detector as described later in this disclosure. This process is generally referred to as a sequencing reaction. This method of preparation is commonly used in preparing molecules for sequencing using electrophoresis. Several variations of this technique exist, are well known and are mostly based on methods proposed by Sanger, F., Nicken, S. and Coulson, A. R. Proc. Natl. Acad. Sci. USA 74, 5463 (1977) and the methods proposed by Maxam, A. M. and Gilbert, W. Methods in Enzymology 65, 499-599 (1980). 
     Referring to the example embodiment in  FIG. 2 , a schematic view is shown of a short strand of DNA prepared using a sequencing reaction.  21  represents the original sequence of nucleotides that is to be analyzed. The ellipses  22 ,  23 ,  24  and  28  indicate the positions of an arbitrary number of intervening bases that are not shown due to space limitations in the drawing. The bases shown in this view are A representing adenine, C representing cytosine, G representing guanine and T representing thymine. The particular sequence shown has no particular significance and was chosen randomly for the purposes of illustration only. The invention does not depend upon any specific bases or number of bases in the molecule under analysis.  20  represents the primer region. The strand shown generally at  25  above and complementary to the original sequence represents the copy of the original sequence generated by PCR. The molecule is shown in the state after the polymerase has completed the copying of the original sequence  21  and the polymerization has been, in an example embodiment, terminated by molecule  27 . The terminating molecule  27  has label  26  attached to it. In the case shown, the terminating molecule is shown as a T and is complimentary to the corresponding molecule A on the original sequence. 
     In the example embodiment, the terminating molecule  27  that is incorporated is a dideoxynucleotide with a fluorophore molecule  26  attached to it. The terminating molecule  27  is shown as a T in this case since T is complimentary to A; this example embodiment was chosen for illustration. The tag molecule  26  in this case is a fluorophore. It emits light when stimulated by an external source such as a laser. The emission spectrum of this molecule is chosen to be unique for the particular terminating molecule that it is attached to. For example the terminating molecule that is complementary to A will have a unique fluorophore that will have a unique emission spectra to the fluorophore that is attached to the terminating molecule complimentary to T and likewise unique for C and G. This allows each terminating molecule to be uniquely identified when stimulated so that they can be differentiated from the other bases. The tag molecule  26  could alternatively be a chromophore or any molecule that will emit a detectable emission when stimulated by an external source and that can be uniquely distinguished from the emissions of the other tag molecules in the sample. The present discussion refers to the analysis of DNA and the bases present therein, however, RNA could be analyzed in a similar fashion. In the case of RNA, it would be necessary to use a terminating molecule that would be complimentary to Uracil and use a polymerase appropriate for the reaction. The present invention is not intended to be limited only to the sequencing of DNA. 
     During the sequencing reaction, a sufficient number of copies of the original sequence are generated to provide sufficient signal for the detector when stimulated. As the molecules are synthesized by the polymerase, the terminating molecules are randomly incorporated which halts extension. The reaction is prepared to produce a generally uniform quantity of copies ranging from the first base to the entire length of the original molecule. 
     The example sequencing reaction for the present invention makes uses of the polymerase chain termination reaction however; any method that yields copies of the original sequence that can be distinguished from the other terminating molecules representing a different base is acceptable. What is important for the process is to have one or more copies of the original sequence for each base in the original sequence and that each copy has a length representative of the position that each base occupies. For example if a molecule having 5 bases were to be analyzed there should be at least 5 molecules with lengths of 1, 2, 3, 4 and 5 nucleotides. Each of the 5 molecules will have a terminating molecule that is complimentary to the original base at the terminating position in the original molecule. The terminating position refers to the position of the base at the location where copying was terminated. 
     In chain terminator sequencing (Sanger sequencing), extension is initiated at a specific site on the template DNA by using a short oligonucleotide ‘primer’ complementary to the template at that region. The oligonucleotide primer is extended using a DNA polymerase, an enzyme that replicates DNA. Included with the primer and DNA polymerase are the four deoxynucleotide bases (DNA building blocks), along with a low concentration of a chain terminating nucleotide (most commonly a di-deoxynucleotide). Limited incorporation of the chain terminating nucleotide by the DNA polymerase results in a series of related DNA fragments that are terminated only at positions where that particular nucleotide is used. The fragments are then size-separated by electrophoresis in a slab polyacrylamide gel, or more commonly now, in a narrow glass tube (capillary) filled with a viscous polymer. 
     The classical chain termination method or Sanger method first involves preparing the DNA to be sequenced as a single strand. The DNA sample is divided into four separate samples. Each of the four samples have a primer, the four normal deoxynucleotides (dATP, dGTP, dCTP and dTTP), DNA polymerase, and only one of the four dideoxynucleotides (ddATP, ddGTP, ddCTP and ddTTP) added to it. The dideoxynucleotides are added in limited quantities. In an example embodiment, the primer or the dideoxynucleotides are either radiolabeled or have a fluorescent tag. 
     As the DNA strand is elongated the DNA polymerase catalyses the joining of deoxynucleotides to the corresponding bases. However, if a dideoxynucleotide is joined to a base, then that fragment of DNA can no longer be elongated since a dideoxynucleotide lacks a crucial 3′-OH group. Fragments of all sizes should be obtained due to the randomness of when a dideoxynucleotide is added. However, to make sure that all different lengths will occur, only short stretches of DNA can be sequenced in one test. 
     The DNA is then denatured and the resulting fragments are separated (with a resolution of just one nucleotide) by gel electrophoresis, from longest to shortest. The shorter fragments have greater mobility in the gel than the longer fragments and therefore arrive at the detector first with successively longer fragments following. Each of the four DNA samples is run on one of four individual lanes (lanes A, T, G, C) depending on which dideoxynucleotide was added. Depending on the whether the primers or dideoxynucleotides were radiolabeled or fluorescently labeled, the DNA bands can be detected by exposure to X-rays or UV-light and the DNA sequence can be directly read off the gel. Bands in the gel indicate the positions of the DNA molecules of different lengths. A band in a lane indicates a chain termination for that particular DNA subunit and the DNA sequence can be read off accordingly. 
     There can be various problems with sequencing through the Sanger Method. The primer used can also be annealed to a second site. This would cause two sequences to be interpreted at the same time. This can be solved by higher annealing temperatures and higher G and C content in the primer. Another problem can occur when RNA contaminates the reaction, which can act like a primer and leads to bands in all lanes at all positions due to non specific priming. Other contaminants can be from other plasmids, inhibitors of DNA polymerase, and low concentrations of template in general. Secondary structure of DNA being read by DNA polymerase can lead to reading problems and will be visualized on the readout by bands in all lanes of only a few positions. 
     There are two sub-types of chain-termination sequencing. In the original method, the nucleotide order of a particular DNA template can be inferred by performing four parallel extension reactions using one of the four chain-terminating bases in each reaction. The DNA fragments are detected by labeling the primer with radioactive phosphorous prior to performing the sequencing reaction. The four reactions would then be run out in four adjacent lanes on a slab polyacrylamide gel. 
     A development of this method used four different fluorescent dye-labeled primers. This has the advantage of avoiding the need for radioactivity; increasing safety and speed, and also that the four reactions can be combined and run in a single gel lane, if they can be distinguished. This approach is known as ‘dye primer sequencing’. 
     An alternative to the labeling the primer is to label the terminators instead, commonly called ‘dye terminator sequencing’. The major advantage of this approach is the complete sequencing set can be performed in a single reaction, rather than the four needed with the labeled-primer approach. This is accomplished by labeling each of the dideoxynucleotide chain-terminators with a separate fluorescent dye, which fluoresces at a different wavelength. This method is easier and quicker than the dye primer approach, but may produce more uneven data peaks (different heights), due to a template dependent difference in the incorporation of the large dye chain-terminators. This problem has been significantly reduced with the introduction of new enzymes and dyes that minimize incorporation variability. 
     This method is now used for the vast majority of sequencing reactions as it is both simpler and cheaper. The major reason for this is that the primers do not have to be separately labeled (which can be a significant expense for a single-use custom primer), although this is less of a concern with frequently used ‘universal’ primers. 
     To produce detectable labeled products from the template DNA, ‘cycle sequencing’ is most commonly performed. This approach uses repeated (25-40) rounds of primer annealing, DNA polymerase extension and disassociation (melting) of the template DNA strands. The major advantages of cycle sequencing is the more efficient use of the expensive sequencing reagent (BigDye) and the ability to sequence templates with strong secondary structures such as hairpins or GC-rich regions. The different stages of cycle sequencing are performed by altering the temperature of the reaction using a PCR thermal cycler. This relies on the fact that complementary DNA will anneal at a lower temperatures and disassociate at higher temperatures. An important part of making this possible is the use of DNA polymerase from a thermophillic organism, which is not rapidly denatured at the high (&gt;95 C) temperatures involved. In the past, new DNA polymerase had to be added individually every cycle of PCR. 
     Various large-scale sequencing strategies include several current methods which can directly sequence only short lengths of DNA at a time. For example, modern sequencing machines using the Sanger method can achieve a maximum of around 1000 base pairs This limitation is due to the geometrically decreasing probability of chain termination at increasing lengths, as well as physical limitations on gel size and resolution. 
     It is often necessary to obtain the sequence of much larger regions. For example, even simple bacterial genomes contain millions of base pairs, and the human genome has more than 3 billion. Several strategies have been devised for large-scale DNA sequencing, including primer walking (see also chromosome walking) and shotgun sequencing. These involve taking many small reads of the DNA through the Sanger method and subsequently assembling them into a contiguous sequence. The different strategies have different tradeoffs in speed and accuracy; for example, the shotgun method is the most practical for sequencing large genomes, but its assembly process is complex and potentially error-prone. 
     It is easier to obtain high quality sequence data when the desired DNA is purified and amplified from any contaminants that may be in the original sample. This can be achieved through PCR if it is practical to design primers that cover the entire desired region. Alternatively, the sample can be cloned using a bacterial vector, harnessing bacteria to “grow” copies of the desired DNA a few thousand base pairs at a time. Most large-scale sequencing efforts involve the preparation of a large library of such clones. 
     Certain areas of molecular biology research are very dependent upon identifying and sequencing RNA. RNA is less stable in the cell, and also more prone to nuclease attack experimentally. As RNA is generated by transcription from DNA, the information is already present in the cell&#39;s DNA. However, it is sometimes desirable to sequence RNA molecules. In particular, in Eukaryotes RNA molecules are not necessarily co-linear with their DNA template, as introns are excised. To sequence RNA, the usual method is first to reverse transcribe the sample to generate DNA fragments. This can then be sequenced as described above. 
     Referring to one example embodiment shown in  FIG. 1 , once a sample has been prepared, it is ready for use. An example embodiment of the present invention comprises a source of nucleic acid fragments each being distinguishable by its spectral characteristics as described above. The example embodiment further comprises a mass dependent molecule isolator which in the current embodiment comprises means for vaporization and acceleration of the nucleic acid fragments shown generally at  1 ; means  17  for introducing the nucleic acid fragments to the vaporization and acceleration means; a drift region  2  having two ends  18  and  19  and having the vaporization and acceleration means  1  located at one end  18  of the drift region and directed so that it propels the nucleic acid fragments through the drift region along the path generally represented by the dashed line  7 ; detecting means shown generally at  3  located at the end  19  of the drift region  2  generally opposite the accelerating and vaporization means  1 . The detecting means  3  comprises means  12  for inducing emission from the nucleic acid fragments represented by the dashed line  7 ; and means  9  for detecting emissions from the tagged nucleic acid fragments, represented schematically by the wavy arrow  10  and distinguishing the tagged nucleic acid fragments. Referring again to  FIG. 1 , the vaporizing and accelerating means  1  in the example embodiment is an electrospray device. The purpose of this device is to vaporize the molecules of the sample and accelerate them to a velocity that is proportional to their masses. Typically with electrospray the molecules of the sample are vaporized, ionized and accelerated by an ion accelerator. The velocity that the molecules are accelerated to is proportional to their mass to charge ratio. Electrospray is a common technique used in mass spectrography for vaporizing and accelerating a sample to be analyzed and is well understood. U.S. Pat. No. 5,015,845 Allen et al., shows such a device. This patent is cited for reference; there are many different designs for this technique that will work well for the purposes of the present invention. Electrospray is used in the example embodiment because it accelerates large molecules without causing significant degradation of the molecules and because it lends itself to a continuous process. With electrospray, the sample can be introduced continuously to the device while maintaining the vacuum in the drift region. This means that the drift region  2  and detector  3  do not have to undergo periodic pump downs just to introduce more samples. This is highly desirable in in achieving high throughput since it eliminates the down time that would be incurred if these chambers had to be pumped down periodically. 
     Vaporization and acceleration of the sample may be accomplished by many other methods. Other methods used for mass spectrography may be used providing different advantages as can be appreciated by those skilled in the art. Some of these methods are Matrix Assisted Laser Desorption Ionization, Fast-atom bombardment, Electron impact, Field ionization, Plasma-desorption ionization or Laser ionization. The particular technique is not important as long as the sample is vaporized so that the molecules are generally separated from each other and that the molecules all receive generally the same amount of energy during acceleration. Another important characteristic of the vaporization and acceleration means  1  is that vaporization and acceleration be accomplished without significant degradation of the sample molecules. Significant degradation of the sample for example, would be a situation in which the sample molecules were broken apart to a degree that prevented an accurate signal to be detected by the detection means  3 . In this situation, the molecules would not be of the correct size to represent the position of the base nucleotide indicated by the attached tag. The molecule would then be accelerated to a velocity inappropriate for the base. Upon reaching the detector, they would contribute noise that would inhibit accurate determination of the base for that position. If the noise signal from the degraded molecules is greater than the proper signal, it would cause inaccurate detection. 
     Referring again to  FIG. 1 , each molecule in the sample is accelerated and allowed to travel down drift region  2  generally along the path indicated by dashed line  7 . The drift region  2  has an chamber area  8  which is generally free of obstruction that would inhibit free travel of the molecules. The chamber  8  is maintained at sufficient vacuum so as not to cause collisions with stray molecules that might cause degradation of the sample molecules or significantly disturb the flight of the sample molecules. A vacuum port is shown generally at  5  and is connected to a vacuum pump capable of maintaining sufficient vacuum as described above. The location of this port is shown generally close to the exit port  14  of the vaporizing and accelerating means. This is to more efficiently remove stray molecules entering the chamber  8  through exit port  14 . The sample molecules will be essentially unaffected. Alternatively, one or more vacuum pumps may be used and positioned anywhere along the drift region as long as they are capable of maintaining sufficient vacuum as described earlier. 
     As the sample molecules travel down the drift region  2 , the smaller (faster moving nucleic acid fragments) move ahead of the larger ones and are thereby sorted sequentially by size.  FIG. 3  shows a hypothetical mixture of sample fragments generally at  40 . The mixture is depicted symbolically to represent a mixture of randomly positioned fragments of different lengths. This is representative of the molecules after vaporization and immediately before acceleration.  FIG. 4  shows the same molecules as depicted in  FIG. 3  shortly after acceleration generally at  50 ,  51 ,  52  and  53 .  FIG. 4  illustrates symbolically the process of separation that occurs due to differing velocities of each different fragment length. The arrow  54  shows the general direction of travel of all of the molecules in the sample. The smallest molecules shown generally at  50  have begun to move ahead of the larger molecules shown generally at  51 ,  52  and  53 . The same is true of the next smallest molecules  51 , which are shown moving ahead of larger molecules at  52  and  53 . Likewise, the molecules at  52  have begun to move ahead of the larger molecules at  53 .  FIG. 5  illustrates symbolically the same molecules depicted in  FIGS. 3 and 4  but at a point in time sufficiently later to allow more complete separation of the molecules. The arrow  64  represents the general direction of travel of the molecules and each different size molecule is represented generally at  60 ,  61 ,  62  and  63  where the smallest molecules are depicted at  60 , next largest at  61 , next largest at  62  and largest at  63 . At this point in time the differences in velocity of each different size molecule has caused a separation and sorting by size to occur. In reality the number of different sized molecules in the sample will usually be more than four as shown in  FIGS. 3 ,  4  and  5 ; however it can be appreciated that for the purposes of illustration, this small number was chosen to more simply illustrate the separation process in a symbolic manner. 
     The length of the drift region  2  as shown in  FIG. 1 , is chosen to allow sufficient distance and time for the molecules to separate sufficiently to allow individual detection of each size molecule. The length of the drift region in the example embodiment is typically 1 to 2 meters but can be longer or shorter depending upon the velocity of the molecules and upon the type of molecule being analyzed. What is important is that the length be sufficient to allow sufficient separation of the molecules for accurate detection by the detector  3 . 
     Referring again to  FIG. 1 , once the molecules reach the end of the drift region  19 , they enter the detector  3 . The detector of the example embodiment includes a vacuum chamber  15  that is generally contiguous with the chamber  8  of the drift region and a vacuum pump connected to port  6 . The vacuum port  6  has a generally curved section  20  where the sample molecules strike after leaving the detector. The curvature of the port at  20  helps slow down the molecules and deflect them to the vacuum pump connected at  6 . 
     The detector  3  also includes means for inducing emission from the sample nucleic acid fragments, which for the example embodiment is a laser  12 . The laser  12  is directed through a transparent window  16  in the wall of the chamber and is aimed to intersect the flight path of the molecules  7  as shown generally at  13 . The wavy arrow  10  is a symbolic representation of the emissions from the molecules as they are illuminated by the laser beam  11 . In the case of the example embodiment, these emissions are photons. The laser has associated optics that focus and condition the emission inducing photons so that they illuminate the sample molecules in a sufficiently narrow region. The size of the region in the direction of travel of the molecules should be narrow enough to prevent significant illumination of neighboring molecules of different sizes and thus avoid stray signals that could give an erroneous reading. The width of the beam in the plane perpendicular to the flight path of the molecules should be sufficient to illuminate enough of the molecules to generate a detectable signal and maximize the signal to noise ratio. The wavelength of the laser is chosen to best coincide with the excitation maxima for all the fluorescent dye molecules in the sample and thus provide a reasonable compromise for optimal emission from all of the fluorophores. 
       FIG. 6  shows a block diagram of the optics for a detector in accordance with the present invention. This view is shown looking parallel to a plane that is perpendicular to the flight path of the sample molecules  7  as shown in  FIG. 1 . Referring to  FIG. 6 , the laser  12  emits a beam of photons that are that focused and conditioned by optics  76  and is directed to illuminate the sample molecules  77 . Some of the photons emitted from the sample are focused and separated into spectral bands by detector optics shown generally at  78 . The detector optics shown in  FIG. 6  includes a lens  71  and a prism  70 . The lens focuses the beam and the prism separates the beam into spectral bands that then strike photomultiplier tubes  72 , 73 , 74  and  75 . 
       FIG. 7  shows a hypothetical stream of molecules symbolically represented by the ovals generally at  80 . Each molecule has a fill pattern that represents the particular tag present in that group of molecules. Group  81  is tagged with the molecule indicating A, group  82  is tagged with the molecule indicating C, group  83  is tagged with the molecule indicating G and group  84  is tagged with the molecule indicating T. Like fill indicates like tags. The lines below the stream labeled Tag 1 (A), Tag 2 (C), Tag 3 (G) and Tag 4 (T) are hypothetical outputs from each of the four detectors  72 , 73 , 74  and  75  that correspond to the tags on the molecules shown generally at  80  above. These outputs illustrate amplitude of the output signal vs. time for each detector. As each group of molecules pass through the laser, they are illuminated causing them to fluoresce. The light emitted passes through lens  71  is refracted by prism  70  and directed to one of the four photomultiplier tubes  72  through  75  depending upon the wavelength of light emitted. 
     The outputs from the photomultiplier tubes are fed into a computer having a high-speed interface to capture the data. As the data comes in from each input, the computer makes the conversion from input source to corresponding base and combines the data sequentially to yield the sequence of the original molecule under analysis. Since the molecules pass the detector in order of increasing size, the order of the out put signals is the same as the order of the original sequence being analyzed. 
     While for the purposes of disclosure and illustration, the example embodiment has been discussed in detail there are numerous other possible components that can be used in combination to achieve the same purposes and still fall within the scope of the invention. Some of these have been listed above and additional possibilities are listed below for illustration purposes. 
     An example embodiment of the invention has been explained for sequencing of nucleic acids such as DNA and RNA. Other example embodiments of the invention will be obvious to those skilled in the art and can be used for sequencing proteins or any polymer or chain type molecule. Common elements in the analysis are:
         a) the molecules analyzed in the apparatus be duplicates of the original molecule;   b) the duplicates have some distinguishing characteristic representative of the original component molecule occupying the end position;   c) and the distinguishing characteristic be induced to emit some detectable signal that is differentiable from other distinguishing characteristics of the other component molecules being analyzed.       

     An example detection means for the invention comprises a laser to induce fluorescent emission from the molecules and a photomultiplier to detect these emissions. Other embodiments could use a light from a source such as an electric lamp, directed at the molecules and optical detectors to measure the absorption of light by the molecules. Still another embodiment might sense the emission from molecules tagged with different chromophores. Other embodiments could sense radio frequency emission from molecular tags that emit a distinguishable RF signal when stimulated. Still other embodiments of the detector could sense higher energy emissions such as X-rays when stimulated. 
     Some alternate methods of stimulation include electron beam, ion beam, and other electro magnetic radiation such as radio frequency, x-ray, ultra violet and gamma ray. High energy collisions with a surface could be used wherein the tag emits radiation of a differentiable spectrum when impact occurs. An example of this is a metal atom incorporated as a tag, and stimulation by a high-energy collision with a surface. 
     Some other example embodiments of methods of isolating the molecule to be analyzed include various techniques employed by mass spectrometry. 
     Mass spectrometry is an analytical technique used to measure the mass of molecules based on mass-to-charge ratio (m/q) of ions generated from the molecules. It is most generally used to find the composition of a physical sample by generating a mass spectrum representing the masses of sample components. Mass spectrometers do this by separating one or more molecules according to their mass and by detecting the molecules after the separation. Based on the detection and separation the mass can be determined. The technique has several applications, including: 
     a) identifying unknown compounds by the mass of the compound and/or fragments thereof. 
     b) determining the isotopic composition of one or more elements in a compound. 
     c) determining the structure of compounds by observing the fragmentation of the compound. 
     d) quantitating the amount of a compound in a sample using carefully designed methods (mass spectrometry is not inherently quantitative). 
     e) studying the fundamentals of gas phase ion chemistry (the chemistry of ions and neutrals in vacuum). 
     f) determining other physical, chemical or even biological properties of compounds with a variety of other approaches. 
     A mass spectrometer is a device used for mass spectrometry, and produces a mass spectrum of a sample to find its composition. This is normally achieved by ionizing the sample and separating ions of differing masses and recording their relative abundance by measuring intensities of ion flux. A typical mass spectrometer comprises three parts: an ion source, a mass analyzer, and a detector. 
     The ion source is the part of the mass spectrometer that ionizes the material under analysis (the analyte). The ions are then transported by magnetic or electrical fields to the mass analyzer. 
     Techniques for ionization have been key to determining what types of samples can be analyzed by mass spectrometry. Electron ionization and chemical ionization are used for gases and vapors. In chemical ionization sources, the analyte is ionized by chemical ion-molecule reactions during collisions in the source. Two techniques often used with liquid and solid biological samples include electrospray ionization (due to John Fenn) and matrix-assisted laser desorption/ionization (MALDI, due to M. Karas and F. Hillenkamp). Inductively coupled plasma sources are used primarily for metal analysis on a wide array of samples types. Others include fast atom bombardment (FAB), thermospray, atmospheric pressure chemical ionization (APCI), secondary ion mass spectrometry (SIMS) and thermal ionization. 
     Mass analyzers separate the ions according to their mass-to-charge ratio (m/q). All mass spectrometers are based on dynamics of charged particles in electric and magnetic fields in vacuum where the following to laws apply: 
         F=q ( E+v×B ), (Lorentz force law) 
       F=ma (Newton&#39;s second law of motion) 
     where F is the force applied to the ion, m is the mass of the ion, a is the acceleration, q is the ionic charge, E is the electric field, and v×B is the vector cross product of the ion velocity and the magnetic field. 
     Using Newton&#39;s third law of motion yields: 
       ( m/q ) a=E+v×B    
     This differential equation is the classic equation of motion of charged particles. Together with the particles initial conditions it completely determines the particles motion in space and time and therefore is the basis of every mass spectrometer. It immediately reveals that two particles with the same physical quantity m/q behave exactly the same. This is why all mass spectrometers actually measure m/q and strictly speaking should be called mass-to-charge spectrometers. In mass spectrometry it is very common to use the dimensionless m/z, where z is the number of elementary charges (e) on the ion (z=q/e) instead of the mass-to-charge ratio m/q. 
     There are many types of mass analyzers, some using static fields, some using dynamic fields, some using magnetic fields, some using electric fields, but all operate according this same law. Several examples are provided as follows: 
     a) Section MS: It uses an electric and/or magnetic field to affect the path and/or velocity of the charged particles in some way. As shown above, sector instruments change the direction of ions that are flying through the mass analyzer. The ions enter a magnetic or electric field which bends the ion paths depending on their mass-to-charge ratios (m/q), deflecting the more charged and faster-moving, lighter ions more. The ions eventually reach the detector and their relative abundances are measured. The analyzer can be used to select a narrow range of m/q&#39;s or to scan through a range of m/q&#39;s to catalog the ions present. 
     Besides the original magnetic-sector analyzers, several other types of analyzer are now more common, including time-of-flight, quadrupole ion trap, quadrupole and Fourier transform ion cyclotron resonance mass analyzers. 
     b) TOFMS: Perhaps the easiest to understand is the Time-of-flight (TOF) analyzer. It boosts ions to the same kinetic energy by passage through an electric field and then measures the times they take to reach the detector. While the nominal kinetic energy of all the ions is the same, the resultant velocity is different, thereby causing lighter ions (and also more highly charged ions) to reach the detector first. 
     c) QMS: Quadrupole mass analyzers use oscillating electrical fields to selectively stabilize or destabilize ions passing through a RF quadrupole field. 
     d) QIT: The quadrupole ion trap works on the same physical principles as the QMS, but the ions are trapped and sequentially ejected. Ions are created and trapped in a mainly quadrupole RF potential and separated by m/q, non-destructively or destructively. There are many mass/charge separation and isolation methods but most commonly used is the mass instability mode in which the RF potential is ramped so that the orbit of ions with a mass a&gt;b are stable while ions with mass b become unstable and are ejected on the z-axis onto a detector. Ions may also be ejected by the resonance excitation method, whereby a supplemental oscillatory excitation voltage is applied to the endcap electrodes, and the trapping voltage amplitude and/or excitation voltage frequency is varied to bring ions into a resonance condition in order of their mass/charge ratio. The cylindrical ion trap mass spectrometer is a derivative of the quadrupole ion trap mass spectrometer. 
     e) Linear QIT: In the linear quadrupole ion trap the ions are trapped in a 2D quadrupole field instead of the 3D quadrupole field of the QIT. 
     f) FTICR: Fourier transform mass spectrometry or more precisely Fourier transform ion cyclotron resonance mass spectrometry measures mass by detecting the image current produced by ions cyclotroning in the presence of a magnetic field. Instead of measuring the deflection of ions with a detector such as a electron multiplier, the ions are injected into a Penning trap (a static electric/magnetic ion trap) where they effectively form part of a circuit. Detectors at fixed positions in space measure the electrical signal of ions which pass near them over time producing cyclical signal. Since the frequency of the ions&#39; cycling is determined by its mass to charge ratio, this can be deconvoluted by performing a Fourier transform on the signal. FTMS has the advantage of improved sensitivity (since each ion is ‘counted’ more than once) as well as much higher resolution and thus precision. 
     g) ICR: Ion cyclotron resonance is an older mass analysis technique that is similar to FTMS above except ions are detected with a traditional detector. Ions trapped in a Penning trap are excited by an RF electric field until they impact the wall of the trap where the detector is located with ions of different mass being resolved in time. 
     h) Orbitrap: Orbitraps are the most recently introduced mass analyzers (commercially available since 2005). Ions are electrostatically trapped in an orbit around a central, spindle-shaped electrode. They perform two kinds of movements in parallel: First, they cycle in an orbit around the central electrode. Second, they also move back and forth along the axis of the central electrode. Thus, the ion movement resembles a ring that oscillates along the axis of the spindle. This oscillation generates an image current in detector plates which is recorded. The frequencies of these image currents depend on the mass to charge ratios of the ions in the Orbitrap. Mass spectra are obtained by Fourier transformation of the recorded image currents. Similar to Fourier transform ion cyclotron resonance mass spectrometers, Orbitraps have a high mass accuracy, high sensitivity and an increased dynamic range. 
     Each of the above analyzer types has its strengths and weaknesses. In addition, there are many more less-common mass analyzers. Many mass spectrometers use two or more mass analyzers for tandem mass spectrometry (MS/MS). 
     The final element of the mass spectrometer is the detector. The detector records the charge induced or current produced when an ion passes by or hits a surface. In a scanning instrument the signal produced in the detector during the course of the scan versus where the instrument is in the scan (at what m/q) will produce a mass spectrum, a record of how many ions of each m/q are present. 
     Typically, some types of electron multiplier is used, though other detectors (such as Faraday cups) have been used. Because the number of ions leaving the mass analyzer at a particular instant is typically quite small, significant amplification is often necessary to get a signal. Microchannel Plate Detectors are commonly used in modern commercial instruments. In FTMS, the detector consists of a pair of metal plates within the mass analyzer region which the ions only pass near. No DC current is produced, only a weak AC image current is produced in a circuit between the plates. 
     Another example embodiment runs 4 differently tagged molecule groups simultaneously. The different emissions from the different tags distinguish between A, C, G and T. Alternately, a single tagged molecule group could be run and the output data could then be combined afterwards to achieve the same results as running  4  simultaneously. Likewise, any combination of tagged molecule groups could be run together to obtain data for the molecules represented by the tags. 
     The invention is well suited to fulfill the objects of the invention. Since the molecules to be analyzed are accelerated to a high velocity to effect separation, the travel time through the apparatus is very short, on the order of 10 −6  seconds. Therefore, the time to analyze a single sample is very small. The samples can be loaded into the vaporizer and accelerator in a way such that the vacuum can be maintained and the next sample can be introduced as soon as the previous sample has fully passed the detector. Once the sample is detected, it enters a scrubbing area where it is deflected and immediately removed by the vacuum pump. This allows almost a continuous flow of samples to be run through the apparatus, which allows for very high throughput. 
     The present invention may or may not rely upon impact type detectors like a micro channel device. In one example embodiment, the present invention does not rely upon impact type detectors like a micro channel device. This means that the detector life does not degrade as a function of sample molecules being run. This provides for significantly longer detector life, higher throughput and the reduction of down time. 
     In addition, the sequence determination may or may not be dependant upon very precise measurements of differences in arrival times of the molecules to distinguish between terminating molecules. In one example embodiment, the sequence determination is not dependant upon very precise measurements of differences in arrival times of the molecules to distinguish between terminating molecules. As molecule size increases the difference in mass between different terminating molecules becomes a very small difference compared to the total mass of the molecule. This makes differentiation much more difficult for larger molecules. Differentiation of the terminating molecule in the present invention is not dependant upon precise measurements in arrival time and therefore is not subject to the problems encountered by mass spectrometry. The present invention is therefore, well suited to determine the sequence of larger molecules with greater accuracy than before. 
       FIG. 10  shows an example embodiment apparatus  100  for analyzing at least one molecule  102  the apparatus comprises: A mass dependent molecule isolator  101  adapted to isolate at least one molecule wherein the isolation depends substantially on the mass of the at least one molecule; a molecule detector  103  in communication with the isolator the molecule detector comprises: at least one source of a radiant signal inducer  104  wherein the radiant signal inducer  105  is emitted continuously from the at least one source and; a signal detector  106  comprising at least one wavelength dependent photon detector. 
     The mass dependent molecule isolator  101  in the present embodiment is a time of flight mass analyzer. It uses an electric field to accelerate ionized molecules through the same potential, and then allows them to drift. If the particles all have the same charge, then their kinetic energies will be identical, and their velocities will depend only on their masses. Lighter ions will reach the detector first. Molecules will therefore be isolated depending substantially upon their mass. 
     The at least one molecule  102  is accelerated in the molecule isolator  101  and allowed to drift along flight path  107  until it reaches the molecule detector  103  where the radiant signal inducer  105 , a laser beam, intersects the flight path and interacts with the molecule  102 . At least one photon  108  is emitted from the molecule  102  as a result of the interaction of the molecule and the signal inducer. The laser beam is emitted from the source of a radiant signal inducer  104  which is a continuous wave laser in the current embodiment and comprises a control system  113 . Continuous emission of the radiant signal inducer from the source ensures interaction with the molecule being analyzed and obviates the need for additional control circuitry to ensure proper interaction. 
     The photon  108  is detected by the signal detector  106 . Data from the signal detector is collected by data collector  112 . The signal detector comprises a wavelength dependent photon detector which comprises a photomultiplier tube  109  and a filter  110  placed in front of the photon receiving portion  111  of the photomultiplier tube. The filter  110  provides the ability to selectively detect photons depending upon the wavelength of the photon. 
     Other embodiments of a wavelength dependent photon detector may be used in the current in invention to accomplish the same result. Another example wavelength dependent photon detector is shown in  FIG. 11  generally at  114  and comprises a diffraction grating  115 , a charge coupled device (CCD)  116 , collimating optics  117  and data collection system  119 . The one or more photons enter the collimating optics  117  and are collimated into a beam  118  which strikes diffraction grating  115 . The diffraction grating directs photons of different wavelengths  118   a  and  118   b  to different locations on the CCD where they generate a signal that is collected by the data collection system  119 . The data from the data collection system then can be selectively used depending upon the wavelength detected as needed. Another example wavelength dependent photon detector is shown in  FIG. 6  comprising detector optics shown generally at  78  including a lens  71  and prism  70 . The lens collimates the signal beam  10  and the prism  70  refracts the signal beam depending upon the wavelength of the photons comprising it. Photomultiplier tubes  72 ,  73 ,  74  and  75  are placed appropriately to receive photons of the desired wavelength. 
     While the current embodiment mass dependent molecule isolator comprises time of flight mass analyzer other mass analyzers may be substituted to accomplish the same result. Other example mass dependent isolators include a quadrupole mass analyzer and a magnetic-sector mass analyzer. 
     The current embodiment radiant signal inducer comprises light from a continuous wave laser however further embodiments may comprise other signal inducers as will occur to those skilled in the art for analysis of a particular molecule of interest. Some examples of other signal inducers include particles and other electromagnetic radiation. 
     The example embodiment shown in  FIG. 10  comprises a method for analyzing at least one molecule. this method comprises Isolating at least one molecule wherein said isolating depends substantially on the mass of the at least one molecule; subsequently Interacting the at least one molecule with a radiant signal inducer  105  wherein the radiant signal inducer is emitted continuously from at least one source  104 ; causing the at least one molecule to emit at least one photon  108  and detecting the at least one photon. The isolating step is performed by mass dependent molecule isolator  101 . The Interacting step occurs when molecule  102  travels along flight path  107  and is struck by radiating signal inducer  105 . The step of causing the at least one molecule to emit a photon happens as a result of the interaction of the radiating signal inducer and the molecule interaction. The detecting step happens as a result of the emitted photon  108  striking the signal detector  106 . 
     Another example embodiment comprises a mass dependent molecule isolator adapted to isolate at least one molecule wherein the isolation depends substantially on the mass of the at least one molecule and a molecule detector in communication with the isolator. The molecule detector of the current embodiment is shown in  FIG. 12  comprises: at least one source of a radiant signal inducer  120 , wherein the radiant signal inducer is emitted from the at least one source and comprises at least two on-pulses  121   a  and  121   b  separated by an off-pulse  121   c ; a duration control system  126  to control the duration of the off-pulse  121   c  to be less than the time that the at least one molecule  122  is in a position to interact with the signal inducer as it travels along flight path  123 ; a photon discriminator  125  comprising at least one wavelength dependent photon detector. 
     The present invention comprises a pulsed radiant signal inducer. A pulsed radiant signal inducer is generated by a pulsed source. A pulsed source in some cases includes advantages such as improved signal to noise ratio and a reduction in component cost. Lower cost components can be used in some instances since a higher power output can be achieved operating in pulsed mode rather than in continuous mode for a given size source. 
     When a pulsed radiant signal inducer is used there is a chance of the molecule to be analyzed passing through the detector without interacting with the radiant signal inducer as illustrated in  FIGS. 13 and 14  and  15 .  FIGS. 13 ,  14  and  15  show an enlarged view of the region where the molecule  122  is in a position to interact with the signal inducer pulses  128   a  and  128   b . The series of figures show a sequence time slices where molecule  122  passes through the region where interaction with the signal inducer is possible but does not occur because the molecule passes through this region at the same time the off-pulse passes through the region.  FIG. 13  shows molecule  122  traveling along flight path  123  and beginning to enter the interaction region  127 . Signal inducer pulse  128   b  has just left the interaction region and signal inducer pulse  128   a  has not yet arrived.  FIG. 14  shows molecule  122  midway through the interaction region  127  while signal inducer pulse  128   a  is still approaching the interaction region but has still not arrived.  FIG. 15  shows molecule  122  exiting the interaction region  127  just before signal inducer pulse  128   a  enters the interaction region. These series of figures illustrate how a molecule can miss interaction with the radiant signal inducer if the duration of the off-pulse is greater than the time that the molecule  122  is in a position  127  to interact with the signal inducer as the molecule travels along its flight path  123 .  FIGS. 16 ,  18  and  19  show similar views to those of  FIGS. 13 ,  14  and  15  however they illustrate the effect of an off-pulse time less than the time that the molecule is in a position to interact with the signal inducer as it travels along its flight path.  FIG. 16  shows molecule  122  traveling along flight path  123  and beginning to enter the interaction region  130 . Signal inducer pulse  129   b  is still in the interaction region and signal inducer pulse  129   a  is just arriving.  FIG. 14  shows molecule  122  midway through the interaction region  130  while signal inducer pulse  129   a  is midway through the interaction region while pulse  129   b  is just leaving the interaction region.  FIG. 15  shows molecule  122  exiting the interaction region  130  and still interacting with signal inducer pulse  129   a . Thus by controlling the duration of the off-pulse so that it is less than the time that the molecule is in a position to interact with the radiant signal inducer detection of the molecule can be ensured. 
     For one example embodiment the time that the molecule is in a position to interact with the radiant signal inducer can be calculated as shown in  FIG. 19 . W is the width of the interaction region which in the present embodiment is the width of the signal inducing beam; d is the diameter of the molecule and v is the velocity of the velocity along the flight path  123 . The time T can be calculated as shown in the formula in  FIG. 19 . 
     An alternate example embodiment molecule detector for use with a pulsed radiant signal inducer is shown in  FIG. 20  generally at  139  and comprises: at least one source of a radiant signal inducer  131  wherein the radiant signal inducer is emitted from the at least one source and comprises at least two off-pulses  133   a  and  133   b  separated by an on-pulse  132   b ; a timing control system  136  to time the emission of the at least one on-pulse  132   b  of the signal inducer to allow interaction with the at lest one molecule  138 ; and a photon discriminator  135  comprising at least one wavelength dependent photon detector. In the present embodiment the molecule is isolated by the mass dependent molecule isolator  210  and travels along flight path  137 . The timing control system receives a signal from the mass dependent molecule isolator  210  which is then used to time the emission of the at least one on-pulse  132   b  of the signal inducer to allow interaction with the at lest one molecule  138 . Without the timing control circuit, the on-pulse might not properly interact with the molecule and proper detection of the signal from the molecule might not occur. 
       FIG. 20  shows an example embodiment apparatus comprising a method for analyzing a property of at least one molecule. The current example embodiment method comprises: Isolating at least one molecule  138  wherein said isolating depends substantially on the mass of the at least one molecule; subsequently Interacting the at least one molecule  138  with a radiant signal inducer  132   b , wherein the signal inducer is emitted from at least one source  131  and comprises at least two off-pulses  133   a  and  133   b  separated by an on-pulse  132   b , wherein the interacting further comprises: determining when the at least one molecule will be in a position to interact with the signal inducer and timing the emission of the at least one on-pulse  132   b  of the signal inducer to allow interaction with the at lest one molecule  138  based on said determining; detecting a signal  134  emitted from the at least one molecule resulting from the interacting of the at least one molecule and the radiant signal inducer  132   b . The step of isolating is performed by the mass dependent molecule isolator  210 . The step of interacting is performed by the travel of the molecule  138  along flight path  137  and intersecting the path of the radiant signal inducer  132   b  and the determining and emission timing steps of the interacting step are performed by the timing control system  136 . The detecting step is performed by the photon discriminator  135 . 
       FIG. 12  illustrates a detector for a further example embodiment comprising a method for analyzing a property of at least one molecule the method comprises: Isolating at least one molecule wherein said isolating depends substantially on the mass of the at least one molecule; subsequently Interacting the at least one molecule with a radiant signal inducer  121   b , wherein the signal inducer is emitted from at least one source  120  and comprises at least two on-pulses  121   a  and  121   b  separated by an off-pulse  121   c , wherein the interacting comprises: determining the amount of time that the at least one molecule will be in a position to interact with the signal inducer and controlling the off-pulse duration to be less than the time that the at least one molecule is in a position to interact with the signal inducer; detecting a signal emitted from the at least one molecule resulting from the interacting of the at least one molecule and the radiant signal inducer. The Isolating step is performed by a mass dependent molecule isolator. The interacting step is performed by the motion of the molecule along flight path  123  so as to intersect the path of the radiating signal inducer  121   b . The determining step can be performed by the manufacturer, the user of the apparatus or automatically by the apparatus of the current embodiment. The step of controlling the off-pulse duration is performed by the duration control system  126 . The step of detecting is performed by the photon discriminator  125 . 
       FIG. 21  shows another alternate example embodiment molecule detector for use with a pulsed radiant signal inducer generally at  150 . This embodiment comprises: at least one source of a radiant signal inducer  142  wherein the radiant signal inducer is emitted from the at least one source and comprises at least two off-pulses  148   a  and  148   b  separated by an on-pulse  147   b ; a timing control system  144  to time the emission of the at least one on-pulse  147   b  of the signal inducer to allow interaction with the at least one molecule  140 ; and a photon discriminator  145  comprising at least one wavelength dependent photon detector. The present embodiment also comprises a second source of a radiant signal inducer  143  that emits a continuous beam of a radiant signal inducer  151  and is directed to intersect the flight path  149  of the molecules at detection point  154 . A second molecule  141  is shown at detection point  154  and emits a signal  152  when interacted with radiant signal inducer  151 . Signal  152  is detected by detector  153 . The signal from detector  153  is communicated to the timing control system  144  and is used to time the emission of the at least one on-pulse to interact properly with the molecule  141  detected at  154  when it arrives at  155   
       FIG. 22  shows an example embodiment molecule detector generally at  165  in communication with the mass dependent molecule isolator  164  comprising; at least one source of a radiant signal inducer  156 ; a signal detector  160 ; and an analyzer  161  in communication with the signal detector  160  configured to supply an output signal that is a function of an input signal  159  and one or more reference values. In the current embodiment, molecule  158  interacts with radiant signal inducer  157  and produces a signal  159 . In the current embodiment, detector  160  detects the absorption of radiant signal inducer  157  by molecule  158  and signal  159  is normally lower when molecule  158  is present than if no molecule is present. One quantitative measure of absorption of a signal can be determined by calculating optical density. 
     Optical density is the absorbance of an optical element for a given wavelength λ per unit distance: 
     
       
         
           
             
               OD 
               λ 
             
             = 
             
               
                 
                   A 
                   λ 
                 
                 l 
               
               = 
               
                 
                   
                     - 
                     
                       1 
                       l 
                     
                   
                    
                   
                     log 
                     10 
                   
                    
                   T 
                 
                 = 
                 
                   
                     1 
                     l 
                   
                    
                   
                     
                       log 
                       10 
                     
                      
                     
                       ( 
                       
                         
                           I 
                           0 
                         
                         I 
                       
                       ) 
                     
                   
                 
               
             
           
         
       
     
     Where: 
     1=the distance that light travels through the sample (i.e., the sample thickness), measured in cm 
     A λ =the absorbance at wavelength λ 
     T=the per-unit transmittance 
     I0=the intensity of the incident light beam 
     I=the intensity of the transmitted light beam 
     Many suitable methods exist (including optical density) for quantitating absorption of a signal and analyzer  161  may be configured to supply an output signal that is a function of an input signal by making use of such methods of calculation. Another method that may be used involves measuring a reference signal that is detected by detector  160  with no molecule present and then subtracting the value of the signal  159  when the molecule is present. The difference will represent a signal value characteristic of the absorption of the molecule. 
     The example embodiment of  FIG. 22  comprises a method for analyzing a property of at least one molecule. The method of the current example embodiment comprises: Isolating at least one molecule wherein said isolating depends substantially on the mass of the at least one molecule  158 ; subsequently Interacting the at least one molecule with a radiant signal inducer  157 ; detecting absorption of at least a part of the radiant signal inducer resulting from the interacting of the at least one molecule and the radiant signal inducer determining at least one property of the at least one molecule based on the detecting. The step of isolating is performed by the mass dependent molecule isolator  164 . The step of interacting is performed when the molecule travels along its flight path  163  and intersects the path of the radiating signal inducer  157 . The step of detecting absorption is performed by the signal detector  160 . The step of determining at least one property is performed by the analyzer  161 . 
       FIG. 23  shows an example embodiment molecule detector generally at  173  in communication with the mass dependent molecule isolator  172  the molecule detector comprises: a radiating signal inducer  167  which in the current embodiment is a particle beam; and a signal detector  171 . The molecule  168  is isolated by the mass dependent molecule isolator  172  and travels along flight path  169  to the detection region generally at  174  where it interacts with the particle beam  167  and produces a signal  170  which is detected by detector  171 . The signal  170  in the current embodiment comprises electromagnetic radiation. In alternate embodiments, the signals detected by detector  171  may comprise electromagnetic radiation or particle radiation and will depend upon the particle type of the radiating signal inducer and the molecule type being analyzed. 
     The example embodiment of  FIG. 23  comprises a method for analyzing a property of at least one molecule. The method of the current example embodiment comprises: Isolating at least one molecule wherein said isolating depends substantially on the mass of the at least one molecule; subsequently Interacting the at least one molecule with a particle beam  167 ; detecting a signal  170  resulting from the interacting of the at least one molecule and the particle beam. The step of isolating is performed by the mass dependent molecule isolator  172 . The step of interacting is performed when the molecule travels along its flight path  169  and intersects the path of the particle beam  167 . The step of detecting is performed by the signal detector  171 . 
       FIG. 24  shows an example embodiment apparatus generally at  175  for determining the sequence of subunits of at least one sample molecule comprising two or more subunits by analyzing two or more fragment groups having two or more fragment molecules  180   a  through  180   d ; each of the two or more fragment molecules having a known subunit in a known position; and each fragment group being prepared using the at least one sample molecule. 
       FIG. 25  shows an example molecule generally at  189  comprising two or more subunits (in this example 7)  188   a  through  188   g , in this case the types of subunits that the molecule comprises are A, B and C.  FIGS. 26 ,  27  and  28  each show different fragment groups.  FIG. 26  shows a fragment group for the A subunit type and has three fragment molecules in its group.  FIG. 27  shows a fragment group for the C subunit type and has two fragment molecules in its group.  FIG. 28  shows a fragment group for the B subunit type and has two fragment molecules in its group. Each of the two or more fragment molecules have a known subunit in a known position. For example the fragment group shown in  FIG. 26  has a known subunit, A at a known position—the right hand end position, these positions are  190   a ,  190   b  and  190   c  on each of the fragment molecules. Likewise, the fragment group shown in  FIG. 27  has a known subunit, C at the right hand end position  191   a  and  191   b  on each of the fragment molecules. Similarly, the fragment group shown in  FIG. 28  has a known subunit, C at the right hand end position  192   a  and  192   b  on each of the fragment molecules. Each of the fragment groups in  FIGS. 26 ,  27  and  28  have been prepared using the molecule shown in  FIG. 25 . Many methods for preparing fragment groups for different molecule types exist and are well known. Some examples include enzymatic methods that use the sample molecule as a template such as the chain terminator sequencing (Sanger sequencing) reaction and the dye terminator sequencing reaction which may be used to prepare fragment groups for DNA. When DNA is sequenced in accordance with the present embodiment, the subunits are adenine, guanine, cytosine and thymine and the known position of the subunit in both dye terminator sequencing and Sanger sequencing is the end position of the fragment. Other methods for generating fragments for other molecules such as proteins RNA and polysaccharides make use of digestion or degradation. 
     Referring again to  FIG. 24  the example embodiment shown generally at  175  comprises: A mass dependent molecule isolator  193 ; a molecule detector  194 ; a time measuring device  185  and an analyzer  195 . 
     The mass dependent molecule isolator  193  is adapted to isolate at least one molecule wherein the isolation depends substantially on the mass of the at least one molecule and comprises: a molecular ionizer  182 ; and a molecular accelerator  183 ; 
     In the present example embodiment the molecular ionizer  182  is a matrix assisted laser desorption ionizer. The shape at  196  schematically represents a molecule sample to be analyzed. Other ionizers such as electro-spray ionizers may be substituted as will be evident to those skilled in the art. The molecular accelerator includes accelerating grid  196  and accelerating control unit  197  and accelerates the molecules after they are ionized by the molecular ionizer. 
     The molecule detector  194  is in communication with the mass dependent molecule isolator  193  and allows the isolated molecules to travel to the detector. The detector comprises at least one source of a radiant signal inducer  176  and a signal detector  178 . The source of a radiant signal inducer in the present invention comprises a laser. The signal detector  178  comprises a photomultiplier tube. 
     The time measuring device  185  measures the time between acceleration of a fragment group by the molecular accelerator  183  and the reception of at least one signal  179  by the signal detector  178 . 
     The analyzer  195  comprises a time measurement recorder  186  and a data processor  187 . The time measurement recorder  186  is configured to record the time measurements made by the time measuring device  185  and to associate the measurements with a corresponding fragment group. 
     The data processor  187  configured to combine time measurements recorded for the two or more fragment groups an place the measurements in time order to thereby indicate at least a part of the sequence of subunits in the at least one sample molecule. 
     When a signal is detected by the molecule detector  194  the time measuring device communicates a time measurement to the time measurement recorder  186  where the data is stored and associated with the corresponding fragment group. In the present example embodiment different fragment groups are run separately and recorded by the time measurement recorder  186 .  FIG. 29  shows a schematic representation of the data recorded by the time measurement recorder. The lanes indicated by  198   a ,  198   b  and  198   c  schematically represent data recorded for each of the fragment groups. Lane  198   a  represents time recordings made for the fragment group representing the A subunits. Lane  198   b  represents time recordings made for the fragment group representing the B subunits. Lane  198   c  represents time recordings made for the fragment group representing the C subunits. The bars such as  199   a  an  199   b  indicate an individual time recording. The arrow labeled “Time” represents the time scale and bars farther right indicate time measurements made later in the run. The bar labeled  199   a , for example, represents a time measurement for a fragment having an A subunit. The bar labeled  199   b , for example, represents a time measurement for a fragment having an B subunit and was detected before bar  199   a  in time. 
     Once all fragment groups have been run, the data processor  187  combines the time measurements recorded for the fragment groups and places the measurements in time order. The process is illustrated schematically in  FIG. 29 . The data processor takes each of the time measurements from each lane and combines them into a single lane  200  in time order to thereby indicate at least a part of the sequence of subunits in the sample molecule.  FIG. 29  represents this process schematically and the concept of lanes has been used to illustrate the data combination process in a visual fashion. For purposes of illustration the sample molecule depicted in  FIG. 29  is shown in  FIG. 25  and each of the fragment groups are shown in  FIGS. 26 ,  27  and  28 . The subunit designation has no significance other that to illustrate the principle. In example embodiments the subunits may be from, for example, DNA, RNA or proteins and may have more or less fragment groups. 
     The example embodiment of  FIG. 24  comprises a method for determining at least one subunit of at least one sample molecule comprising two or more subunits. The method of the current example embodiment comprises: Isolating at least one fragment molecule  180   c  having a known subunit in a known position of the fragment molecule wherein the fragment molecule has been prepared using the at least one sample molecule, wherein said isolating depends substantially on the mass of the at least one fragment molecule; subsequently Interacting the at least one fragment molecule  180   c  with a radiant signal inducer  177 ; detecting a portion of the radiant signal inducer scattered  179  as a result of the interacting of the at least one fragment molecule and the radiant signal inducer; determining at least a part of the sequence of subunits based on the detecting. The step of isolating is performed by the mass dependent molecule isolator  193 . The step of interacting is performed when the molecule travels along its flight path  181  and intersects the path of the radiating signal inducer  177 . The step of detecting is performed by the signal detector  178 . The step of determining at least a part of the sequence of subunits is performed by the analyzer  195 . 
       FIG. 30  shows an example embodiment generally at  208  comprising a mass dependent molecule isolator  202  adapted to isolate at least one molecule wherein the isolation depends substantially on the mass of the at least one molecule and a molecule detector  209  in communication with the isolator. 
     The mass dependent molecule isolator  202  in the current embodiment comprises a Fourier transform ion cyclotron resonance molecule isolator and further comprises a Fourier transform ion cyclotron resonance mass analyzer similar to that used in a Fourier transform ion cyclotron resonance mass spectrometer. In this type of molecule isolator the molecules are accelerated and allowed to circulate in a circular path as shown by  203   a    203   b  and  203   c . The circulation of the ions on this path depends upon the mass-to-charge ratio (m/z) of the ions based on the cyclotron frequency of the ions in the fixed magnetic field of the molecule isolator. Isolation of molecules in this detector occurs spatially as illustrated by the concentric paths  203   a ,  203   b  and  203   c.    
     The detector  209  comprises a source of radiant signal inducer  201 , a continuous wave laser in the present embodiment and a signal detector  205 . The laser emits a radiant signal inducer  207 , the laser beam that intersects the ion paths  203   a ,  203   b  and  203   c . The interaction of the molecule ions with the radiant signal inducer  207  generates signals  204   a ,  204   b  and  204   c  that are detected by the signal detector  205 . An analyzer unit  206  process the signals received by the detector  205  and performs a furrier transform on the data to deconvolute the data and associate it with its appropriate molecule. 
       FIG. 1A  shows an example embodiment detector in cross-section view. This example embodiment detector is configured to detect a signal emitted from the molecule  13   a  who&#39;s flight path is perpendicular to the plane of the drawing. The detector comprises a source of a radiant signal inducer  12   a ; and photomultiplier tube  9   a . The radiant signal inducer interacts with the molecule  13   a  and emits a signal  10   a  that is detected by photomultiplier tube  9   a . The configuration shown in  FIG. 1A  is illustrative of the configuration comprised in the example embodiment of  FIG. 1 . 
       FIG. 1B  shows an example embodiment detector in cross-section view. This example embodiment detector is configured to detect a signal absorbed by the molecule  13   b  who&#39;s flight path is perpendicular to the plane of the drawing. The detector comprises a source of a radiant signal inducer  12   b ; and photomultiplier tube  9   b . The radiant signal inducer interacts with the molecule  13   b  and absorbs part of the radiant signal inducer to generate a signal  10   b  that is detected by photomultiplier tube  9   b.    
       FIG. 1C  shows an example embodiment detector in cross-section view. This example embodiment detector is configured to detect a signal scattered from the molecule  13   c  who&#39;s flight path is perpendicular to the plane of the drawing. The detector comprises a source of a radiant signal inducer  12   c ; and photomultiplier tube  9   c . The radiant signal inducer interacts with the molecule  13   c  and scatters a signal  95   a  that is detected by photomultiplier tube  9   c.    
     The present invention is capable of very high throughput, requires less maintenance and can be easily automated. This means that sequencing and molecular analysis can be performed at a significantly higher rate with fewer machines at substantially lower cost. This makes the invention well suited for large-scale sequencing and molecular analysis. 
     The present invention is well adapted to carry out the objects and attain the ends and advantages mentioned, as well as others inherent therein. While, for the purposes of disclosure there have been shown and described what are considered at present to be the example embodiments of the present invention, it will be appreciated by those skilled in the art that other uses may be resorted to and changes may be made to the details of construction, combination of shapes, size or arrangement of the parts, or other characteristics without departing from the spirit and scope of the invention. It is therefore desired that the invention not be limited to these embodiments, and it is intended that the appended claims cover all such modifications as fall within the true spirit and scope of the invention. 
     REFERENCES 
     The following references, to the extent that they provide exemplary procedural or other details supplementary to those set forth herein, are specifically incorporated herein by reference.
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     Various articles or publications include the following:
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Parr, Michael C. Fitagerald and Lloyd M. Smith. (1992). Matrix-assisted Laser Desorption/Ionization Mass Spectrometry of Synthetic Oligodeoxyribonucleotides. Rapid Communications in Mass Spectrometry, Vol. 6, 369-372.   Lloyd M. Smith. (1993). The Future of DNA Sequencing. Science, Vol. 262, 530-532.   Michael C. Fitzgerald, Lin Zhu and Lloyd M. Smith. (1993). The Analysis of Mock DNA Sequencing Reactions Using Matris-assisted Laser Desorption/Ionization Mass Spectrometry. Rapid Communications in Mass Spectrometry, Vol. 7, 895-897.   Christine M. Nelson, Lin Zhu, Wei Tang, Lloyd M. Smith, Kevin Crellin, Jamal Berry and Jesse L. Beauchamp. ( ). Fragmentation Mechanisms of Oligonucleotides in MALDI Mass Spectrometry.   Chad C. Nelson, Lesa M. Nelson and Kenneth Ward. ( ). Large-Scale Populationh Screening of Genetic Variants using ESI/MS Analysis of Multiplex PCR Products. Dept. of Human Genetics, University of Utah, Salt Lake City, Utah.   Huaiqin Wu and Hoda Aboleneen. ( ). 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Nucleic Acids Research, 2002, Vol. 30, No. 21 e117. Institute of Biochemistry, Medical Faculty, University of Leipzig, Liebigstrasse 16, D-04103 Leipzig, Germany. *To whom correspondence should be addressed. Tel: +49 341 9722105; Fax: +49 341 9739371; Email: eschrich@uni-leipzig.de http://nar.oxfordjournals.org/cgi/content/abstract/30/21/e117   John R. Edwards, Yasuhiro Itagaki and Jingyue Ju *(2001). DNA sequencing using biotinylated dideoxynucleotides and mass spectrometry. Nucleic Acids Research, 2001, Vol. 29, No. 21 e104. http://nar.oxfordjournals.org/cgi/content/full/29/21/e104   Kai Tang*, Dong-Jing Fu \ , Dominique Julien, Andreas Braun, Charles R. Cantor, and Hubert Köster (1999). Biochemistry Chip-based genotyping by mass spectrometry (DNA chip/single nucleotide polymorphism) Vol. 96, Issue 18, 10016-10020, Aug. 31, 1999. Sequenom Inc., 11555 Sorrento Valley Road, San Diego, Calif. 92121. Contributed by Charles R. 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