Abstract:
The present invention is directed to systems and methods of providing universal quantum computation that avoid certain external control fields that either are hard or impossible to implement, or are serious sources of decoherence (errors). The systems and methods extend the set of scalable physical platforms suitable for implementing quantum computation in solid state, condensed matter and atomic and molecular physics systems. The invention includes identifying of suitable encodings of logical qubits into three physical qubits—i.e. three quantum mechanical systems of two levels—and performing quantum computing operations by changing the quantum states of physical qubits making up one or more logical qubits using only generalized anisotropic exchange interactions. This includes performing a quantum unitary operation over a single logical qubit or a non-local (entangling) two-qubit unitary operation. An exemplary embodiment of the invention uses a physical qubit represented by two electronic quantum levels of a nanoparticle supported in an electromagnetic cavity. The physical qubit, i.e. its quantum levels can be tuned by electromagnetic field from a pulsed laser, so that the qubit can be brought into the interaction (resonance) with another physical qubit via exchange of cavity quantum electromagnetic modes.

Description:
CLAIM OF PRIORITY  
       [0001]     This patent application claims priority from U.S. Provisional Patent Application No. 60/455,395, filed on Mar. 18, 2003. 
     
    
     STATEMENT OF GOVERNMENT RIGHTS  
       [0002]     This invention was made with U.S. government support under grant N00014-01-1-0826 awarded by the U.S. Office of Naval Research and under AF Agreement F30602-01-2-0524 awarded by the U.S. Air Force Research Laboratory. Accordingly, the United States government has certain rights in the invention. 
     
    
     TECHNICAL FIELD  
       [0003]     This invention relates to computation, and more specifically to quantum computation and quantum information processing.  
       BACKGROUND ART  
       [0004]     Quantum mechanical systems have been investigated for numerous applications known as quantum information processing including quantum computation, quantum communication and quantum cryptography. A quantum system can be used to store and very efficiently process information which is carried in its two-state quantum subsystems, called quantum bits or “qubits.” The computation and information processing based on quantum mechanical principles can outperform classical computation and information processing in a number of tasks like database search and prime factorization problems.  
         [0005]     A quantum computer is particularly attractive tool if it is “universal,” that is, capable of solving any computable task. Quantum computation is known to be universal as long as arbitrary single-qubit and non-local (entangling) two-qubit unitary operations can be applied in an arbitrarily structured sequence called a quantum circuit. These operations are a result of the physical structure of the system and control fields applied on it, which both are embodied in the Hamiltonian of the system. Universality is thus determined fundamentally by the physical structure of the qubit implementation and by control of this with clear distinction between controlling an interaction that is intrinsic to the system, and introducing a new interaction with an external control field. In many of the possible physical implementations (for details on proposed implementations, see for instance S. L. Braunstein and H. K. Lo, “Scalable quantum computers, paving the way to realization”, Wiley-VCH, 2001), the inherent physical interactions do not suffice to generate the universal set of quantum computing operations over physical qubits and must be supplemented by such additional. external Hamiltonian control terms. This may introduce demanding nanoscale engineering constraints as well as additional unwanted sources of decoherence (i.e. a noise process which destroys the effectiveness of a quantum computer). Consequently, the question of whether and how we can use a particular physical system containing some very specific, non-generic interactions, for universal quantum computation has become very relevant with increasing technological effort in the area of implementation of quantum computation.  
         [0006]     The solution of the problem of a lack of universality of numerous intrinsic physical interactions can be constructed by a suitable encoding of the states representing quantum logic into a two and higher dimensional subspace of the system Hilbert space. This concept is called “encoded universality”. The significance of the encoded universality schemes for quantum computation lies in the fact that they require active manipulation of only two-particle exchange interactions, and hence can be generically referred to “exchange-only computation”, and hence avoid other sources of decoherence like application of additional control fields. They are closely related to numerous proposals for quantum computation in solid state systems in which the exchange interaction is a common feature.  
       SUMMARY OF THE INVENTION  
       [0007]     The present invention has industrial utility with regard to systems for and methods of quantum computing. The present invention is directed to such systems and methods that allow for universal quantum computation that avoid external control fields as sources of decoherence. The systems and methods have industrial utility in extending the set of scalable physical platforms suitable for implementing quantum computation in a solid state environment In summary, an encoding of logical qubits into three physical qubits (i.e. three quantum mechanical systems of two levels) and methods is presented to perform (1) any quantum unitary operation over a single logical qubit and (2) a non-local (entangling) two-qubit unitary operation, specifically C(Z), using only multi-body interaction (i.e. generalized anisotropic exchange interaction). This set of quantum operations is known to be universal. The present invention thus provides a method for universal quantum computation.  
         [0008]     An aspect of the present invention is a system and method for quantum computation using only the generalized exchange interaction between qubits comprising the steps of defining a Hilbert space to represent a physical system; defining encoding of logical qubits into this physical system and storing the quantum information; selecting a set of quantum observables for this system; defining the transformations between encoded logical qubits including both single qubit and two qubit quantum operations; providing the most appropriate architecture for implementation of encoded quantum information and its manipulations; providing the sequences of elementary operations to implement the single qubit and two qubit gates.  
         [0009]     Another aspect of the invention is a system and method for quantum computation using only the generalized exchange interaction between qubits comprising defining a Hilbert space to represent a physical system; defining encoding of logical qubits into this physical system and storing the quantum information; selecting a set of quantum observables for this system; defining the transformations between encoded logical qubits including both single qubit and two qubit quantum operations; providing the most appropriate architecture for implementation of encoded quantum information and its manipulations; providing the sequences of elementary operations to implement the single qubit and two qubit gates.  
         [0010]     Another aspect of the invention is an apparatus and method to perform universal quantum computing by defining all universal encodings of quantum information, constructing the initial states for quantum computation, defining the appropriate quantum computer architecture, and processing the quantum information using the quantum mechanical system by controlling multi-body interactions.  
         [0011]     Physical systems for implementation of quantum computation include solid state systems, e.g., quantum nanoparticles interacting via cavity field or atoms fixed in a solid state crystal (e.g. silicon), trapped ions, neutral atoms in optical lattices, NMR machines including solid state NMR techniques, superconducting electronics, and electrons flowing on helium surface. See for example S. L. Braunstein and H.-K. Lo, “Scalable quantum computers, paving the way to realization”, Wiley-VCH, 2001, the teaching of which are incorporated herein by reference (see http://www.wiley-vch.de/books/tis/eng/3-527-40321-3.html).  
         [0012]     The present invention also provides an apparatus and method for performing universal quantum computation on the DFS by controlling only multi-body interactions in a physical system which by itself is not universal and hence does not suffice to construct a quantum computer. This interaction is relevant to a number of the recent proposals for solid state implementation of quantum computation when additional physical effects such as symmetry breaking perturbations, originating for instance from surface and interface effects, spin-orbit coupling (Dzyaloshinski-Moriya term), dipole-dipole coupling in the spin-spin interaction, and anisotropy in the exciton exchange interaction in quantum dots are taken into account. The asymmetric anisotropic interaction including these cross-terms is also a part of quantum computation with fermionic systems such as quantum states of electrons.  
         [0013]     As discussed below, a preferred example of an apparatus for forming a physical embodiment of the invention for performing universal quantum computation, is an apparatus consisting of n quantum nanoparticles (e.g. atoms, molecules, quantum dots, etc.) localized on a microscopic cavity which mediates their interactions, and a controller for providing predetermined sequences of pulses of frequencies, durations and intensities (power levels) intended to excite the nanoparticles into any state inside 2 n  dimensional Hilbert space.  
     
    
     BRIEF DESCRIPTION OF DRAWINGS  
       [0014]      FIG. 1  is a schematic side-view diagram showing an exemplary embodiment of an apparatus according to the invention, the apparatus having a number of quantum nanoparticles localized on a microscopic cavity whose interaction via a cavity field is controlled by laser fields;  
         [0015]      FIGS. 2A and 2B  are schematic diagrams illustrating the actions of the asymmetric anisotropic exchange interactions over the three qubit code spaces according to an exemplary embodiment of the invention, wherein the solid arrows transform code words via the symmetric component of the Hamiltonian, while the dashed arrows transform code words through its antisymmetric part, wherein the former changes the bit-string parity and preserves the occupation number while the latter changes the occupation number by two while conserving the parity, with the indexes indicating which physical qubits are coupled;  
         [0016]      FIG. 3  is a schematic diagram of the layout of an exemplary scalable architecture according to the invention for a two qubit entangling operation, wherein a controlled-Z gate is implemented using the physical qubits connecting two logical qubits within the layout, e.g. physical qubits  2 - 3 - 4 ; and  
         [0017]      FIG. 4  is a schematic diagram of an example embodiment of a quantum circuit illustrating the pulse sequence for generating encoded single qubit operations. 
     
    
     DETAILED DESCRIPTION  
       [0000]     Generalized Anisotropic Exchange Interaction  
         [0018]     The present invention is directed to universal quantum computation with physical systems whose quantum bits interact via the generalized anisotropic exchange interaction. The Hamiltonian, i.e., the observable describing this interaction, allows asymmetry in the exchange tensor, i.e., J zz =0, J xx ≠J yy , and also incorporates additional cross-terms, σ α   i σ α   j , α≠β. The total interaction can then be described as follows, 
 
 H   ij =(½)Σ α=x,y   J   αα   ij σ α   i σ α   j +(½)Σ α≠β=x,y   J   αβ   ij σ α   i σ β   j    (1) 
 
 where J ij  is the strength of the interaction between qubits whose upper index (αα or αβ) indicates the character of the term (i.e. xx, yy, xy or yx), and σ α are the Pauli matrices. 
 
         [0019]     This asymmetric anisotropic Hamiltonian can be seen to split into two distinct parts that act on orthogonal two-dimensional sectors of the four-dimensional Hilbert space 
 
 H   ij   =J   s   ij   +J   a   ij   +K   s   ij   +K   a   ij ==(½)[ J   s   ij (σ x   i σ x   j +σ x   i σ x   j )+ J   a   ij (σ x   i σ x   j −σ x   i σ x   j )+ K   s   ij (σ x   i σ y   j −σ y   i σ x   j )+ K   a   ij (σ x   i σ y   j −σ y   i σ x   j )]  (2) 
 
where  J   s   jj =( J   xx   ij   +J   yy   ij )/2 , J   a   ij =(J xx   ij   −J   yy   ij )/2 , K   s   ij =( J   xy   ij   +J   yx   ij )/2 , J   a   ij =( J   xy   ij   −J   yx   ij )/2. 
 
         [0020]     These sectors are characterized by the parity of the bit string which refers to even or odd occupation number defined as the number of 1&#39;s in the bit string. In particular, the symmetric terms J s   ij  and K s   ij  operates in the subspace spanned by          ={|01&gt;,10&gt;}, and the antisymmetric term J a   ij  and K a   ij  in the subspace spanned by @={|00&gt;,|11&gt;}. The symmetric term of the Hamiltonian preserves the occupation number and is used in this invention for processing of quantum information, while the antisymmetric changes this occupation number by two and is used in this invention for initialization of the physical qubits for quantum computation. In particular, the symmetric component of the interaction (indexed “s”) acts only in          , and the antisymmetric part (indexed “a”) only in @. In each of the two subspaces the interaction is characterized by the expression J k   ij σ x     +K k   ij σ y     , where the index k is either s or a. This can be reformulated as J k   ij σ +     +J k * ij σ   , where the effective coupling is now a complex number, 
 
 J   k   ij   =J   k   ij   −i K   k   ij    (3) 
 
         [0021]     The operators σ x     , σ y     , σ +     , and σ −      now apply to the pairs of states within any of the two-dimensional subspaces           and @.  
       Exemplary Embodiments of the Invention  
       [0022]     The present invention employs the generalized anisotropic exchange interaction for quantum information processing, including universal quantum computation. Since this interaction is not by itself universal, the present invention extends the number of physical systems which can be used for realization of a quantum computer. Since this interaction is also the result of imperfections and symmetry breaking conditions in quantum computer fabrication, the present invention also allows elimination of these undesired effects.  
         [0023]     The origin of the asymmetry in the anisotropic interaction can be understood as a consequence of energy non-conserving terms in the system Hamiltonian. The antisymmetric terms (J a  and K a ) represents an energy non-conserving process similar to the anti-rotating wave terms arising in the interaction of a two-level system with semiclassical radiation, but happening now in a correlated way on both coupled physical qubits. We may assume that asymmetry in the anisotropic exchange interaction between physical systems is a consequence of the system complexity when numerous mechanisms of mutual coupling take place simultaneously. An example of similar symmetry breaking in the case of the isotropic (Heisenberg) exchange interaction between quantum dots derives from the spin-orbit or a (usually weaker) dipole-dipole coupling.  
         [0024]     This interaction is relevant to a number of the recent proposals for solid state implementation of quantum computation when additional physical effects such as symmetry breaking perturbations, originating, for instance, from surface and interface effects, spin-orbit coupling (Dzyaloshinski-Moriya term), dipole-dipole coupling in the spin-spin interaction, and anisotropy in exciton exchange interaction in quantum dots are taken into account. The asymmetric anisotropic interaction including these cross-terms is also a feature of quantum computation using fermionic systems, such as quantum states of electrons.  
         [0000]     Nanoparticles Interacting Via Cavity Quantum Fields  
         [0025]     An exemplary embodiment of a universal quantum computing apparatus  100  according to the present invention is schematically illustrated in  FIG. 1 . Apparatus  100  includes, along an optical axis A 1 , a pulsed laser source  102  having a wavelength, pulse duration and power suitable for addressing electronic and nuclear levels of nanoparticles (e.g., atoms, molecules, quantum dots, etc.). A collimating lens  104  is arranged to receive radiation  105  from the pulsed laser and form a collimated beam  107  of radiation  105 . Apparatus  100  includes a spatial light modulator  116  arranged to receive the collimated radiation at an input side  116 A and output modulated radiation at an output side  116 B. A suitable spatial light modulator is, for example, a commercially available one-dimensional or two-dimensional 128-pixel or 256-pixel modulator, available from Meadowlark Optics, Inc. Spatial light modulator is operably coupled to a controller  118 , which is also connected to laser source  102  and controls the operation of apparatus  100 .  
         [0026]     Apparatus  100  further includes optical fiber sections  120  each having an input end  120 A and an output end  120 B. Optical fiber sections  120  are optically coupled to modulator output side  116 B at respective pixels so that the light passing through each pixel is communicated to a corresponding optical fiber section. A microcavity  130  is arranged downstream of the spatial light modulator  116 . Microcavity  130  is adapted to support nanoparticles  132  (e.g., atoms, molecules, quantum dots, etc.) in a manner that allows for a controlled exchange interaction between the nanoparticles. The output ends  120 B of the optical fibers are operably coupled to the nanoparticles  132  supported in microcavity  130  so that the laser radiation  105  can interact with the nanoparticles.  
         [0027]     In the operation of apparatus  100 , a physical qubit is, for example, represented by two distinct electronic levels of a nanoparticle  132 . The electronic levels of the nanoparticle are manipulated by the electromagnetic field of the laser radiation  105  carried to the nanoparticle by optical fiber sections  120 . Microcavities and interaction between nanoparticles mediated by cavity fields are subjects of intense experimental research. See, for example, the web page of the experimental group by Evelyn Hu at the University of California at Santa Barbara http://www.cnsi.ucsb.edu/directory/faculty/hu/hu.html. More details, including illustrations about these projects, can be found at http://online.kitp.ucsb.edu/online/nano01/hu/oh/09.html).  
         [0028]     Thus, apparatus  100  creates a controlled exchange interaction between nanoparticles  132  via quantized modes of an electromagnetic field (“laser field”) inside a suitably fabricated microcavity  130  (including, for example, microdisc, circular and spherical cavities). Pairs of electronic levels of two different nanoparticles  132 , defining two distinct quantum bits, are brought into the exchange interaction by tuning these levels into resonance with the cavity modes using the external pulsed laser field of radiation  105 . This operation corresponds to quantum information processing.  
         [0029]     In addition, in an example embodiment, initialization of the quantum states of the encoded logical qubit is carried out using the same interaction but exploiting its antisymmetric component. In order to determine the final state of the quantum computer, the measurement of the logical qubits is carried via detection of its constituents, physical qubits. Once the encoding of a logical qubit is defined, the state of the logical qubit can be uniquely determined by detecting the state of only one specific physical qubit from the code word. This can be carried out, for example, by selective fluorescent detection used in other known implementations of quantum computation (e.g., trapped ions, neutral atoms in optical lattices, etc.). Determining spin by a nuclear magnetic resonance (NMR) technique may also be used in a exemplary embodiment of the invention.  
         [0030]     Other exemplary embodiments of apparatus  100  can be based, for example, on different solid state platforms, trapped ions, trapped neutral atoms interacting via a cavity fields, and superconducting qubits, all of which are currently a subject of profound experimental investigation.  
         [0000]     Universal Codes  
         [0031]     The minimal set of physical qubits for which the asymmetric anisotropic exchange Hamiltonians between neighboring physical qubits can generate universal set of quantum computing operations, consists of three qubits. The Hilbert space describing all physical states of this three qubit system is spanned by eight orthogonal wavefunctions (note that 8=2 3 ). Each of these states is thus characterized by a string of three bits. Under the interaction, the Hilbert space splits into two four dimensional subspaces,          =           4 ⊕           4 , which are characterized by different bit-string parities. These subspaces are not mixed by the interaction Hamiltonian (1), which preserves the bit-string parity (i.e. the number of one&#39;s in the bit string). The four-dimensional subspaces thus define two independent codes that are spanned by the following two sets of code words: 
 
Code (I)={|000&gt;,|110&gt;,|101&gt;,|011&gt;}Code (II)={|111&gt;,|001&gt;,|010&gt;,|100&gt;}  (4) 
 
 with even and odd number of one&#39;s. 
 
         [0032]     Each physical qubit of the code word corresponds to a quantum system of two levels. These are represented by any two distinct quantum states of a complex quantum system (e.g., atoms, molecules, nanoparticles, electrons, etc.), which, in the case of nanoparticles, may for instance be two distinct electronic states characterized by wavefunctions of different orientation of electronic spin. The value “0” and “1” of the quantum bit (qubit) may then correspond to the parallel and antiparallel spin orientation with respect to a suitably chosen axis. For example, these can be defined as |0&gt;=|S=½,m z =−½&gt; and |1&gt;=|S=½,m z =+½&gt; where the axis z is chosen for the spin projection m z  of the system of total spin S=½. A logical qubit can in principle be defined as any pair of these states, although for quantum information processing it is advantageous to use only states of identical occupation number from each of the code spaces. For instance, the logical qubit can be encoded as 
 
|0 L &gt;=|101 &gt;=|S= ½ ,m   z =½&gt; 1   |S= ½ ,m   z =−½&gt; 2   |S= ½ ,m   z =½&gt; 3  
 
and 
 
|1 L &gt;=|011 &gt;=|S= ½ ,m   z =−½&gt; 1   |S= ½ ,m   z =½&gt; 2   |S=  1 / 2     ,m   z =½&gt; 3 , 
 
 where the lower index (1, 2 and 3) indicates the physical qubits. 
 
 Single-Qubit Operations 
 
 Asynimetric Anisotropic Exchange 
 
         [0033]     The Hamiltonian (without cross terms) is applied to the pairs of physical qubits  1 - 2 ,  1 - 3 , and  2 - 3 , in the three qubit codes ( 4 ). The effect of this interaction is the same for both codes, i.e. for (I) and for (II) as the Hamiltonian acts simultaneously and identically on both subspaces            4 , without mixing them. It can therefore be expressed as a direct sum of two 4×4 matrices in the basis of the codes (I) and (II). In the code basis ( 4 ), the effect of the asymmetric anisotropic exchange interaction, schematically summarized in  FIGS. 2A and 2B . For example, the Hamiltonian matrix H 12  represents the coupling between the physical qubits  1  and  2  via its symmetric and antisymmetric components (characterized by the coupling strengths J s  and J a ). The earlier simultaneously transforms the logical qubits |000&gt; and |110&gt; in the code space (I), and |111&gt; and |001&gt; in the code (II); while the latter simultaneously transforms the logical qubits |011&gt; and |101&gt; in the code space (I), and |100&gt; and |010&gt; in the code (II). Similarly, the Hamiltonian H 23  generates transformation between the qubits  2  and  3  within three physical qubits of the code; and the matrix H 13  generates transformation between the physical qubits  1  and  3 .  
         [0034]     Let us now consider the action of these three matrices and of their commutators. We start with H 12 =(J a σ x )⊕ (J s σ x ). It is evident that the symmetric component of H 12  (with coupling strength J s ) acts as a σ x   34  operation over the code words the states |101&gt; and |011&gt; from the code (I), and over the states |010&gt; and |100&gt; from (II), i.e. it acts as encoded  σ   x  on the states in both (I) and (II). The antisymmetric component of H 12  acts on the other two orthogonal states from the code, namely on |000&gt; and |110&gt; from (I), or on |111&gt; and |001&gt; from (II). This also results in an encoded  σ   x  operation but with coupling strength J a . This is the first element required for an encoded SU( 2 ) operation necessary for universal quantum computation.  
         [0035]     The second element is an encoded  σ   y  operation. These operations are generated through the commutator of a pair of Hamiltonian matrices. For instance, taking the commutator of interactions between physical qubits  1 - 3  and qubits  2 - 3  yields [H 13 , H 23 ]=i (J a2 −J s2 )σ y   34 , where σ y   34  acts exclusively on the states |101&gt; and |011&gt;. Since all other elements of the resulting 4×4 matrix are equal to zero, this commutation relation results exclusively in an encoded  σ   y  operator between the code words  3  and  4  from the code (I) and (II).  
         [0036]     The third and last element required for an encoded SU( 2 ) operation is encoded  σ   z . These operations are now obtainable from a second level commutator, namely of the Hamiltonian matrix with the encoded  σ   y  operations. For example, [H 12 ,σ y   34 ]=i2J s σ z   34 .  
         [0037]     Together, these three encoded  σ   x ,  σ   y , and  σ   z  operations ensure that any arbitrary SU( 2 ) operation may be performed on the encoded qubits. We note that the Hamiltonian matrices always act simultaneously on both sets of orthogonal subspaces (I) and (II). We can use the encoded operations described above to generate additional encoded  σ   x  operations that do not simultaneously act on the orthogonal subspaces from the code, by forming the commutator between the  σ   y  and  σ   z  operators.  
         [0038]     Analogous sets of operators can be defined starting from the other two exchange Hamiltonians, i.e., H 13  and H 23 . The connections resulting from all of Hamiltonian interactions and their commutators are equivalent in each case. In total therefore, we have three distinct ways of defining the logical qubit from each of the subspaces (I) and (II), with arbitrary SU( 2 ) operations possible on any of these six possible sets of qubits. From the subspaces (I) the possible encodings are {|110&gt;,|011&gt;}, or {|110&gt;,|101&gt;}, or {|101&gt;,|011&gt;}. From the subspace (II) the possible qubit encodings are {|001&gt;,|100&gt;}, and {|001&gt;,|010&gt;}, and {|010&gt;,|100&gt;}. These encodings make stored logical qubits protected against decoherence, namely collective dephasing error generated by the operator (½)Σ k=1   3 σ z   k .  
         [0000]     Cross-Product Terms  
         [0039]     The inclusion of the cross-product terms transforms the Hamiltonian matrices from the previous section into hermitian matrices of the same structure whose coupling coefficients J a =J a   ij /2 and J s =J s   ij /2 are now complex (see (3)). In fact, the situation captured in the Hamiltonian is the most general anisotropic exchange form containing asymmetry in all terms including the cross-products. It provides a generalization of the usual symmetric anisotropic exchange referred to as an XY model.  
         [0040]     Under these circumstances, application of the commutation relations between the Hamiltonian matrices is still capable of generating the SU( 2 ) algebra for single qubit operations necessary for universal quantum compution. The result of the commutation relation is again proportional to the  σ   y  operation. For instance, [H 13 ,H 23 ]=(|J a | 2 −|J s | 2 )σ y   34 . On the other hand, elementary matrix algebra shows that now only two of three possible commutation relations between pairs of complex Hamiltonian matrices of the three-qubit code can eliminate the coupling between states of different occupation number and thereby generate this encoded  σ   y . The commutation relation which does not generate this transformation is [H 12 , H 23 ]. The universal encodings of a logical qubit are then: {|110&gt;,|101&gt;}, or {|101&gt;,|011&gt;} from the subspace (I), and {|001&gt;,|010&gt;}, and {|010&gt;,|100&gt;} from the subspace (II).  
         [0000]     Two-Qubit Operations  
         [0041]     An entangling two-qubit gate—namely the controlled-Z (C(Z)) operation—is obtained via the following sequence of encoded  σ   z  operations: 
 
 U   C(Z) =exp( i   σ   z   1 π/4) exp( i   σ   z   2 π/4) exp[− i ( σ   z   1   {circle around (x )}σ z   2 )π/4]  (5) 
 
 The crucial element of this sequence is the last term on the right hand side. This is enacted by applying the encoded  σ   z  operation onto the triplet of physical qubits  2 - 3 - 4  that connects two logical qubits within the triangular architecture (see  FIG. 3 ). To illustrate this C(Z) sequence, we focus on an example with the following encoding of logical qubits: |0 L &gt;=|110&gt;, |1 L &gt;=|011&gt;. The logical two-qubit configurations are then given as 
 
|0 L 0 L &gt;=|110110&gt;|0 L 1 L &gt;=|110011&gt;|1 L 0 L &gt;=|011110&gt;|1 L 1 L &gt;=|011011&gt;  (6) 
 
 where the bold fonts indicate those physical qubits which are ‘bridging’ two logical qubits. Via commutation relations of the exchange Hamiltonians between the physical qubits  2 - 4  and  3 - 4  within the triangular architecture ( FIG. 3 ) we generate the σ y   2-3  operation which, when commuted further with the exchange interaction between the qubits  2  and  3 , results in the corresponding σ z  operation. Turning this σ z  operation on for the duration t=π/2 results in a phase transformation of the states, such that |0 L 0 L &gt;=|110110&gt;→e −iπ/2 |0 L 0 L &gt; and |0 L 1 L &gt;=|110011&gt;→e iπ/2 |0 L 1 L &gt;. The other two states are not addressed by the encoded operation and remain intact. The resulting diagonal transformation over the logical two-qubit states, characterized by diagonal elements {−i,i,1,1}, has provided the desired entanglement between the logical qubits. We emphasize that we needed one double commutator to obtain this transformation. In order to illustrate that this suffices to generate the controlled-Z operation, we first apply an encoded  σ   z  onto the second logical qubit for duration t=π/4. This further transforms the relative phase relations between the states of two logical qubits to {−i,1,1,−i} (up to an overall phase e −iπ/4 ). This result is equivalent to the unitary transformation exp[−i( σ   z   1   {circle around (x )}σ z   2 )π/4] in (5). This transformation, when supplemented by the encoded single qubit  σ   z  rotations on both logical qubits, results in the desired controlled-Z operation, C(Z). 
 
 Decoherence Properties 
 
         [0042]     Decoherence is a noise process in quantum computing which may destroy the significant effectiveness of quantum computation compared to classical computation. This process results from coupling of logical qubits into the environment in which quantum information is lost to the environment. It is therefore highly advantageous to provide conditions under which the effect of decoherence is limited or eliminated. The residual decoherence can be eliminated by the process known as error correction (U.S. Pat. No. 6,128,764 to Gottesman discusses quantum computation).  
         [0043]     The encodings, presented in this invention, are eigenvectors with identical eigenvalues of the operator (½)Σ k=1   3 σ z   k . This operator (also known as the parity operator) generates the error (decoherence) process known as collective dephasing. As long as the quantum information is stored in these encodings, it is protected against this class of error; during quantum computing operations the information is not necessarily protected. The invention presents a method for storing quantum information in decoherence free subsystem of a quantum mechanical system of three physical qubits in the case of collective dephasing error.  
         [0000]     Implementation  
         [0000]     Initialization of a Quantum Computer According to the Invention  
         [0044]     In exemplary embodiments of the invention, the initial state of physical qubits of the code (usually |000&gt;) may be initialized to a desired value of the encoded logical qubit (usually |0 L &gt;). The latter can be represented either by any state with two “1” from the code (I) or any state with one ”1” from the code (II). Starting from the state |000&gt;, for example, the desired |0 L &gt;=|110&gt; is provided by application of the anisotropic interaction on the first and second physical qubits for the duration of time given as π/2J a . This pulsed interaction just inverts the values of the first two physical qubits, and thus initializes the desired state of the logical qubit. Similarly, the same pulsed interaction can be applied on any other pair of physical qubits in order to provide any of the other alternatives for encoding logical qubit.  
         [0000]     Quantum Information Processing  
         [0045]     Exemplary embodiments of universal quantum computation according to the invention, featuring generalized anisotropic exchange interactions, are considered as applications of the theoretical development of encoded universality with this class of Hamiltonians into an appropriate quantum circuit. A practical question is implementation of the commutation relations. Previously considered implementation procedure via the Baker-Hausdorff-Campbell operator expansion does not necessarily provide the efficiency required in practical implementation.  
         [0046]     A useful approach according to the invention is based on conjugation by unitary operations, which is embodied in a short sequence of coupling operations, i.e. a quantum circuit, such as illustrated in  FIG. 4 . In the present invention, a short quantum circuit is formulated which provides the same effect over the encoded qubit as exponentiated commutation relations, and thus establishes equivalence between both. The complication due to the presence of the antisymmetric terms in the Hamiltonian matrices is eliminated by choosing a suitable duration of the exchange interaction. Since [J s   ij ,J a   ij ]=0 for any physical qubits i and j, the unitary evolution operator generated by the Hamiltonian (1) splits into a product U(τ)=exp(−i J s   ij  τ) exp(−i J a   ij  τ). For a suitably chosen time duration, one of the terms can always be made to generate the identity, if J s   ij ≠J a   ij . At the same time, the effect of the other term can be tuned to provide desired transformation.  
         [0000]     Single Qubit Operations According to the Invention  
         [0047]     This feature of turning off the undesired effect of the antisymmetric terms in the evolution operator by judicious choice of conjugation operations, is illustrated by an exemplary method according to the invention. For example, the unitary evolution generated by the σ y   34  operator, resulting from the commutation relation [H 13 , H 23 ], can be obtained from the following conjugation: 
 
 U (σ y   34 ,φ)=exp( −i σ y   34 φ)=exp( i H   13 Θ)exp( i H   23 φ′)exp( −i H   13 Θ)   (7) 
 
 where φ′=φ/J s , and Θ is the time duration satisfying simultaneously the two conjugation conditions 
 
Θ=0(mod π)/J a =(π/2)(mod π)/J s    (8) 
 
         [0048]     Due to the asymmetry of the exchange coupling terms (J s ≠J a ) and to the unitarity of the quantum evolution, this condition can easily be fulfilled, as long as the ratio of J s  and J a  is not a rational number. The conjugating operation is implemented directly by a sequence of appropriately timed laser pulses focused on a pair of quantum nanoparticles localized on a microdisc cavity, as illustrated in  FIG. 4 .  
         [0049]     The second conjugation needed for  σ   z  operations, implementing the double commutator (Section \ref{sec:onequbit}), is carried out in a similar fashion: 
 
 U(σ   z   34 ,φ)=exp( −i σ z   34 φ)=exp( i H   12 θ) U (σ y   34 ,φ)exp( −i H   12 θ)   (9) 
 
         [0050]     Here U(σ y   34 ,φ) is the result of the first conjugation given by Eq. (7). In this exemplary embodiment of the invention, the condition for the time duration of the second conjugating operation generated by H 12  reads as θ=0(mod π)/J s =(π/4)(mod π)/J s . Both conjugations used for construction of single qubit operations are illustrated, for example, in  FIG. 4  as a quantum circuit together with the sequences of operations (e.g. laser pulses) on the physical qubits of an encoded logical qubit.  
         [0051]     Development of a conjugating procedure for the case of the general Hamiltonian, containing the cross-product terms, is carried out within the same framework. However the relevant timing conditions have to reflect that the coupling coefficients J a  and J s  may now be complex numbers. Just as in the previous case, the goal is to generate the desired conjugating unitary transformation by exponentiating the appropriate general Hamiltonian operator, where the symmetric part of the interaction leads to exchange between the two coupled code words phase-shifted by imaginary unit i, and the antisymmetric term results in identity. We first illustrate new timing conditions derived from focusing only on the antisymmetric term in the generalized anisotropic exchange.  
         [0052]     The antisymmetric coupling acts on the state with even bit-string parity, @={|00&gt;,|11&gt;}. It can be reformulated as the sum J a σ x   @ +K a σ y   @  where σ y   @  and σ x   @  refer only to the even parity states. In order to establish the conjugating condition, this operator is exponentiated and factorized into the product of three unitary operators exp(−i J a σ x Θ) exp(−i K a σ y Θ) exp(i J a K a σ z Θ/2). The condition for attaining the identity is then: 
 
Θ=0(mod π)/ J   a =0(mod π)/ K   a =0(mod π)/( J   a   K   a /2)   (10) 
 
         [0053]     Considering now in addition that the coupling coefficient J s  is complex and its imaginary part is also to be eliminated, an analogous timing condition can easily be formulated.  
         [0000]     Two Qubit Operations  
         [0054]     We now focus on specific aspects of implementation of the two-qubit gates via conjugation. The entangling part of the controlled-Z gate, described above, is obtained as a conditional effect of the σ z  operation on the physical qubits of both logical qubits (on the ‘bridging’ qubits, see  FIG. 3 ). The conjugation however complicates the situation, due to its antisymmetric component which affects also the states |1 L 0 L &gt;=|011110&gt; and |1 L 1 L &gt;=|011011&gt;. However, the effect of the antisymmetric term in the interaction can be completely eliminated by imposing an additional timing condition for the conjugated operation. In the present example, this operation is generated by H 23 , and the timing condition is then given as follows: 
 
φ′=0(mod π)/ J   a =φ(mod 2π)/ J   s    (11) 
 
 We emphasize that this condition has to be satisfied only up to an arbitrary global phase. 
 
 Efficiency 
 
         [0055]     The method according to the invention based on conjugation is much more effective than application of the Baker-Hausdorff-Campbell formula whose asymptotic character translates into a sequence of a large number of elementary operations. In contrast, in the method according to the invention, the conjugation features three gates for implementation of the encoded  σ   y  operation, emulating a single commutation relation, and five gates for encoded  σ   z , corresponding to a double commutator as illustrated, for example, in  FIG. 4 . The entangling two-qubit operation according to the invention, i.e. the controlled-Z up to the local transformations, is based on generating  σ   z , and hence requires also just five discrete gates. The timing conditions, expressed in number of gates (8) and (10), translate into a prolonged transformation of the conjugating unitaries. It should be pointed out that the duration of the conjugating operation, given by the ratio of the coupling coefficients J a  and J s  in (8), for example, does not change if a larger number of logical qubits defined with this three-qubit encoding are addressed with these gate sequences. Therefore, embodiments of the present invention scale well with respect to size, having only a linear cost in terms of computational complexity as the number of encoded qubits increases.  
         [0056]     Alternative embodiments of the invention, in addition to the present analytical approach featuring conjugation, feature numerical optimization of gate sequences in order to generate the desired quantum computing operations.  
         [0000]     Architecture  
         [0057]     Since the encoded  σ   y  interactions for a given Hamiltonian are defined through the commutation relations with the other two available couplings among three physical qubits, an advantageous architecture for embodiments of the invention is triangular. An equilateral triangular architecture is convenient wherever the coupling between physical qubits is distance dependent, as it ensures that J s  and J a  are the same within any pair of physical qubits taken from a three qubit code, resulting then in pulses of identical durations for any of the coupling. The equilaterality of the triangular architecture is however not a requirement and can be relaxed into any arrangement. The implementation of commutation relations between exchange Hamiltonains via unitary conjugation allows for a number of other architecture structures than equilateral triangle. The change in the coupling strengths (J s  and J a ) between physical qubits, which may result from other architectures, would translate into different durations of the conjugating operations as the same timing conditions (see paragraphs above) are satisfied. In fact, this flexibility is an advantageous aspect of the present invention because it allows one to relax the requirement of an equilateral triangular architecture, to a lattice of a rectangular or any other structure in order to accommodate physical and experimental requirements.  
         [0058]     To accommodate additionally two-qubit logical operations, exemplary embodiments of the invention feature arrangements of triangles of physical qubits into a linear chain with alternating triangle orientations. This layout is shown in  FIG. 3 . Exemplary embodiments of the invention featuring other layouts, such as a hexagonal or cubic lattice, may also be employed under suitable change of durations of conjugating operations.