Device for deriving a change of time-dependent information

Abstract: Time-dependent information such as light whose intensity varies with time is converted into positional information representing the change of the time-dependent information. A series of photoelectrons provided as the time-dependent information are accelerated when passing through a region (d₁) defined by first and second electrodes (11, 12) to which a ramp voltage is applied so that the photoelectrons are accelerated and are released at speeds varying in dependence upon their time of emission. A speed analyzer (13) analyzes the speeds of the photoelectrons and converts this into positional information. The positional information is applied to a phosphor screen (17) on which the positions of the photoelectrons applied to it are displayed. The positions on the screen represent the times of emission of the photoelectrons.

Description: The present invention relates generally to a device for deriving a change of time-dependent information. More particularly, the invention relates to such a device in which time-dependent intensity information or time-dependent quantity information of charged particles such as electrons, ions or the like are converted to positional information spatially representing the times involved with the time-dependent information. The present invention further relates to a device for measuring and displaying a light intensity waveform of light whose intensity varies dependent on time. There have been known (see EP-A- 0 187 087) some devices for measuring time-dependent changes in charged particles in a vacuum, i.e., time-dependent changes in the number of charged particles, in which employed is an electron multiplier. More specifically, the charged particles to be measured are introduced into an electron multiplier and the number of electrons is increased by producing secondary electrons that are liberated upon collision of the charged particles. The electrons are received by an anode and measured by an oscilloscope. According to another arrangement, the charged particles to be measured are caused to impinge on a scintillator and converted thereby into light, which is then detected as an electric signal with a photomultiplier tube (PMT) or the like. The detected electric signal is measured by an oscilloscope. In either of the above conventional devices, a change in the intensity of the charged particles is merely amplified and detected as an electric signal to be measured with an oscilloscope, without effecting any special conversion process with respect to time. Therefore, intensity changes that can be measured are limited by the response speed of the oscilloscope used. It is impossible at present to measure time-dependent intensity changes in less than 30 ps. Even to maintain a response speed of about 30 ps, care should be taken to design the layout of signal lines and select circuit components. It is therefore not easy to measure time-dependent intensity changes in 30 ps. There has been proposed an arrangement based on the principles of a streak tube for a higher response speed, as shown in FIG. 1 of the accompanying drawings. In FIG. 1, two deflection plates 2, 3 are disposed in a path 1 of the charged particles (photoelectrons) to be measured, and a ramp voltage synchronous with the introduced electrons is applied between the deflection plates 2, 3 to convert a time-dependent change in the intensity of the photoelectrons into positional information on an input surface of a microchannel plate 4. The positional information can be visually recognized as light intensities on a phosphor surface 5. The proposed arrangement is effective to increase the response speed greatly compared with the conventional devices. The present invention has been made to provide a new and novel arrangement for deriving a change of time-dependent information. According to one aspect of the present invention, there is provided a device for deriving a change of time-dependent information represented by a series of charged particles, comprising: a source for emitting the charged particles; accelerating or decelerating means for accelerating or decelerating the charged particles emitted from said source and releasing the charged particles at speeds varying in dependence upon the times of their emission; and, analyzing means for analyzing the speeds of the released charged particles and providing output information varying in dependence on the speeds of the charged particles, the output information representing the change of the time-dependent information. The device may further comprise a first voltage source for supplying a voltage varying with time, wherein the accelerating means comprises first and second electrodes disposed in confronting relation to each other, a time--dependent intensity variable electric field being developed between the first and second electrodes in accordance with the voltage from the first voltage source. The analyzing means comprises an output screen such as phosphor screen on which the positional information is applied, the output screen displaying the positions of the charged particles applied thereto, the positions thereof representing the times involved with the charged particles. Since the electric field developed between the first and second electrodes varies with time, the charged particles are given different amounts of energy or speeds dependent on the time at which they are emitted from the charged particle emitting source. Consequently, upon performing an analysis of the energy or speeds of the charged particles with the analyzing means, the change of the time-dependent information can be obtained. According to another aspect of the present invention, there is provided a device for measuring an intensity waveform of light whose intensity varies dependent on time, comprising: photoelectric converting means having a surface for emitting a series of photoelectrons depending on the intensity of the light applied to it; accelerating or decelerating means disposed in confronting relation to the surface of said photoelectric converting means for accelerating or decelerating the photoelectrons emitted from the surface of said photoelectric converting means and releasing the photoelectrons at speeds varying in dependence upon the times of their emission; and, analyzing means for analyzing the speeds of the released photoelectrons and providing output information varying dependent on the speeds of the photoelectrons, the output information representing the intensity of light varying dependent on time. The device may further comprise computing means for computing the positional information and outputting information regarding the light intensity waveform of the light, and displaying means for displaying the intensity waveform of the light based on the information supplied from the computing means. The present invention will be better understood from the following description, given by way of example with reference to the accompanying drawings in which: FIG. 1 is a sectional side elevational view schematically showing a structure of a conventional charged particle measuring device; FIG. 2A is a sectional side elevational view schematically showing a structure of a charged particle measuring device according to an embodiment of the present invention; FIG. 2B is a sectional side elevational view showing a modification of the structure shown in FIG. 2A; FIG. 3 is a diagram showing the waveform of an accelerating voltage applied between a charged particle source and an accelerating electrode; and FIG. 4 is a sectional side elevational view schematically showing a structure of a light intensity waveform measuring device according to an embodiment of the present invention. A first embodiment of the present invention will now be described with reference to FIG. 2A where shown is an arrangement of a charged particle measuring device. The measuring device includes a source 11 for emitting the charged particles, a mesh-like accelerating electrode 12, and a unit 13 serving generally as an energy analyzer and specifically as speed analyzer. The latter two 12, 13 are successively disposed in front of the source 11. A voltage that varies with time is applied between the accelerating electrode 12 and the source 11 by a power supply 14. The potential of one of the source 11 and the accelerating electrode 12 is fixed, whereas the potential of the other varies with time. The energy or speed analyzer 13 includes two deflection plates 15, 16 arranged in parallel to each other with a space therebetween, and an output screen 17 such as a phosphor screen which emits light in response to the charged particles impinged thereon. The analyzer 13 is disposed in an orientation to receive the charged particles through an aperture formed on one face of an enclosure of the analyzer 13. A constant voltage is applied between the deflection plates 15, 16 to develop an electrostatic field in the space therebetween. Charged particles which are entered from the aperture 18 pass through the electrostatic field, and are deflected thereby before reaching the output screen 17. In operation, since the voltage applied to the accelerating electrode 12 varies with time, the intensity of the electric field developed between the source 11 and the accelerating electrode 12 varies in timed relation to the voltage applied to the accelerating electrode 12. Consequently, the charged particles emitted from the source 11 at different times are given different amounts of energy by the electric field, and reach the analyzer 13 at different speeds. On the other hand, an amount by which the charged particle is deflected when passing through the electrostatic field between the deflection plates 15, 16, varies depending on the speed or energy of the charged particle. Therefore, the charged particles that have been emitted from the source 11 at different times reach different positions on the output screen 17. Stated differently, the time-dependent information of the charged particles is converted into positional information on the output screen 17. High-speed changes in the electric field between the source 11 and the accelerating electrode 12 are produced by the power supply 14 which applies a voltage that varies at high speed. According to the recent technology, it is possible to produce a change of 3 kV/200 picoseconds (ps) in the electric field, and hence a voltage change of 0.15 V in 10 femtoseconds (fs). The analyzer 13, on the other hand, has a resolution of 0.1 eV or less. Consequently, less than 10 fs response speed can be achieved by the device of the present invention. Operation of the present embodiment will be described in far more detail while using equations. It is assumed that the charged particle source 11 and the accelerating electrode 12 are spaced from each other by a distance d₁ (zone 1), and the accelerating electrode 12 and the aperture 18 of the analyzer 13 are spaced from each other by a distance d₂ (zone 2). A constant voltage of - V₀ is applied to the source 11, and a ramp voltage is applied to the accelerating electrode 12. The ramp voltage has a waveform such that it varies linearly from 0 volt at a time of t = 0 to a voltage of - V₀ volt at a time t = t f as shown in FIG. 3. The equation of motion of a charged particle that is emitted at the time t = t₀ is given as follows. For the zone 1, d 2 z dt 2 = - Q M · - V 0 - V ( t + t 0 ) d 1 For the zone 2, d 2 z dt 2 = - Q M · V ( t + t 0 + t d1 ) d 2 V ( t ) = -V 0 · t t f where M is the mass of a charged particle, - Q is the electric charge of a charged particle, t d1 , is the time at which the charged particle reaches the accelerating electrode 12. Integrating equations (1) and (2), the speed v and the position z of the charged particle are obtained. For the zone 1, v = dz dt = QV 0 Md 1 t f {( t f - t 0 ) t - 1 2 t 2 } z= QV 0 Md 1 t f {( 1 2 ( t f - t 0 ) t 2 - 1 6 t 3 } For the zone 2, v= QV 0 Md 2 t f ·{( t 0 + t d1 ) t+ 1 2 t 2 } + V d z= QV 0 Md 2 t f ·{ 1 2 ( t 0 + t d ) t 2 + 1 6 t 3 } + V d t + d 1 where V d is the speed in the position z = d₁. Note that the potential at the face of the analyzer enclosure on which the aperture 18 is formed is maintained at 0 volt. For the sake of brevity, it is assumed that the charged particles are electrons, and the parameters are selected as follows: d₁ = 2 mm, d₂ = 0.5 mm, V₀ = 3 kV, and t f = 200 ps, and the electrons emitted successively at the times t₀ = 1ps, t₀ = 2ps, and t₀ = 3ps are applied to the analyzer 13 with the following respective amounts of energy: t₀(ps) Energy (eV) 1 3894 2 3899 3 3903 If these electrons enter between the deflection plates 12, 13 that have a length of ℓ and are spaced from each other by a distance d₃, and a deflection voltage V d is applied between the deflection plates 15, 16, then the amounts Y by which the electrons are deflected on the output screen 17 that is spaced from the deflection plates 15, 16 by a distance of L are given as follows: Y = ℓ V d 2 d 3 V ( ℓ 2 + L ) where V is the energy with which the electrons are applied. If ℓ = 25 mm, d₃ = 5 mm, L = 100 mm, and V d = 1500 volts, then the amounts by which the three electrons that have been emitted at different times are deflected are as follows: t₀(ps) Y (mm) 1 108.3 2 108.2 3 108.1 Therefore, the time-dependent information of the charged particles are converted into positional information on the output screen 17. The time-dependent information of the charged particles can be accessed from the distribution of brightness on the output screen 17. While the accelerating electrode 12 and the analyzer 13 are separate from each other in the above embodiment, the entrance face of the analyzer enclosure may double as an accelerating electrode. In the above embodiment, the power supply 14 serving as a means for applying a variable voltage is connected between the accelerating electrode 12 and the charged particle source 11, and these components jointly serve as an accelerating means for applying an accelerating energy which varies with time. However, the charged particle source 11 may be separate from the accelerating means. FIG. 2B shows such a modification in which the accelerating means for applying a variable accelerating energy includes accelerating electrodes 21, 22 and the variable voltage power supply 14. A constant voltage is applied to an accelerating electrode 23 with respect to the voltage at the source 11 for imparting a constant accelerating energy to the charged particles emitted from the source 11. FIG. 4 shows a second embodiment of the present invention. Shown in Fig. 4 is a light intensity waveform measuring device incorporating therein the time-dependent change measuring device of the present invention. The light intensity waveform measuring device employs a photoelectric transducer means as the charged particle source, and serves to measure the waveform of a time-dependent intensity of light that falls on the photoelectric transducer means. When light 34 to be measured is applied to a photocathode 33, which serves as the photoelectric transducer means, through an aperture 32 in an input window 31, the photocathode 33 emits photoelectrons depending on the intensity of the light applied. When a ramp voltage is applied between the photocathode 33 and the accelerating electrode 35, the photoelectrons emitted from the photocathode 33 are subjected to speed modulation, and pass through an accelerating electrode 35. The electrons then pass through a focusing electrode assembly 36. Time-dependent information of the photoelectrons, i.e., the waveform of a time-dependent intensity of the applied light, is converted into positional information by a speed analyzer 37. The analyzer 37 includes a pair of deflecting plates 38 between which a constant voltage is applied, and an output screen 39. The focusing electrode assembly 36 serves to converge the photoelectrons onto the output screen 39 through adjustment of a voltage applied thereto. During operation, the voltage applied to the focusing electrode assembly 36 remains constant and hence unchanged, so that the modulated velocities of the photoelectrons are not disturbed by the electric field developed by the focusing electrode assembly 36. The output screen 39 is made up of a microchannel plate (MCP) 40 and a phosphor screen 41. The phosphor screen 41 is optically coupled to a CCD (charge coupled device) image sensor 43 through optical fibers 42. Accordingly, light emitted from the phosphor screen 41 can electrically be read as image information which bears intensity information on pixel basis by the CCD image sensor 43. The image information represents the waveform of the time-dependent intensity of the applied light, and may be processed by a computer 45 for displaying it on a display monitor 44. The speed analyzer 37 has a response speed of 25 fs if its energy resolution is 0.5 eV. While it is possible to employ an analyzer having a higher resolution, the time resolution of the light intensity waveform measuring device is limited to the above value because the distribution of initial-speed energies possessed by photoelectrons when they are emitted from the photocathode 33 is about 0.5 eV with respect to a wavelength 500 nm of applied light. In the above embodiment, the photocathode 33 is used as one of the electrodes of the accelerating means which applies a variable accelerating energy. However, as with the embodiments shown in FIGS. 2A and 2B, the photocathode 33 may be separate from the accelerating means by adding a new electrode. In all the above-described embodiments, the accelerating voltage may vary such that it decreases with time rather than increasing with time. The illustrated analyzers employ parallel flat deflection plates. However, a cylindrical energy analyzer, a concentric hemispherical energy analyzer or the like which finds usual use may also be employed. Furthermore, the illustrated deflecting means for developing an electric field in the analyzer may be replaced with a deflecting means for developing a magnetic field. The charged particle measuring device according to the present invention can produce time-dependent information of charged particles at a response speed of several tens fs by modulating the speed of the charged particles with an electric field. The light intensity waveform measuring device which incorporates the charged particle measuring device with a photoelectric transducer means serving as its charged particle source is capable of measuring time-dependent changes in the intensity of light also at a very high response speed of several tens fs. In the embodiments described, whilst an accelerating means is described disposed next to the charged particle emitting source or photoelectric converting means, a decelerating means may be used instead disposed in place of it for decelerating the charged particles or photoelectrons.

Claims: A device for deriving a change of time-dependent information represented by a series of charged particles, comprising: a source (11) for emitting the charged particles; accelerating or decelerating means (12) for accelerating or decelerating the charged particles emitted from said source (11) and releasing the charged particles at speeds varying in dependence upon the times of their emission; and, analyzing means (13) for analyzing the speeds of the released charged particles and providing output information varying in dependence on the speeds of the charged particles, the output information representing the change of the time-dependent information. A device for measuring an intensity waveform of light whose intensity varies dependent on time, comprising: photoelectric converting means (33) having a surface for emitting a series of photoelectrons depending on the intensity of the light applied to it; accelerating or decelerating means (35) disposed in confronting relation to the surface of said photoelectric converting means (33) for accelerating or decelerating the photoelectrons emitted from the surface of said photoelectric converting means (33) and releasing the photoelectrons at speeds varying in dependence upon the times of their emission; and, analyzing means (37) for analyzing the speeds of the released photoelectrons and providing output information varying dependent on the speeds of the photoelectrons, the output information representing the intensity of light varying dependent on time. A device according to claim 2, further comprising computing means (45) for computing the output information and outputting information regarding the light intensity waveform of the light, and displaying means (44) for displaying the intensity waveform of the light based on the information supplied from said computing means (45). A device according to any one of the preceding claims, further comprising a first voltage source (V d ) for supplying a voltage varying with time, and wherein the accelerating or decelerating means (12) comprises first and second electrodes (15,16,38) disposed in confronting relation to each other, a time-dependent intensity variable electric field being developed between the first and second electrodes (15,16,38) in accordance with the voltage from the first voltage source (V d ). A device according to any one of the preceding claims, wherein the analyzing means (13,37) comprises an output screen (17,40) on which the output information is applied, the output screen (17,40) displaying the positions of the charged particles and their positions representing the times involved with the charged particles. A device according to claim 5, wherein the output screen is a phosphor screen (17,40). A device according to any one of claims 4 to 6, wherein the source (11) for emitting the charged particles doubles as the first electrode (15). A device according to any of the preceding claims, wherein the analyzing means (13,37) comprises deflecting means (15,16,38) for deflecting the charged particles in a direction perpendicular to a direction in which the charged particles advance. A device according to claim 8, wherein the analyzing means (13,37) further comprises a second voltage source for applying a constant voltage to the deflecting means (15,16,38) to develop an electrostatic field, the deflecting means imparting a force on the charged particles to deflect in the direction perpendicular to the direction in which the charged particles advance, the force being determined by the electrostatic field. A device according to any one of the preceding claims, wherein the reflecting means imparts a force on the charged particles to deflect in the direction perpendicular to the direction in which the charged particles advance, the force being determined by a magnetic field.

Inventors: SUYAMA MOTOHIRO, SUYAMA, MOTOHIRO, SUYAMA, MOTOHIRO, C/O HAMAMATSU PHOTONICS K.K.
Applicants: HAMAMATSU PHOTONICS KK, HAMAMATSU PHOTONICS K.K.
Application year: 1991
Main classification: H01J31
IPC codes: H01J31, G01T1, G01J1