Quantum simulation of a three-body-interaction Hamiltonian on an NMR quantum computer
被引:98
作者:
Tseng, CH
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机构:MIT, Dept Nucl Engn, Cambridge, MA 02139 USA
Tseng, CH
Somaroo, S
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机构:MIT, Dept Nucl Engn, Cambridge, MA 02139 USA
Somaroo, S
Sharf, Y
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机构:MIT, Dept Nucl Engn, Cambridge, MA 02139 USA
Sharf, Y
Knill, E
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机构:MIT, Dept Nucl Engn, Cambridge, MA 02139 USA
Knill, E
Laflamme, R
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机构:MIT, Dept Nucl Engn, Cambridge, MA 02139 USA
Laflamme, R
Havel, TF
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机构:MIT, Dept Nucl Engn, Cambridge, MA 02139 USA
Havel, TF
Cory, DG
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机构:
MIT, Dept Nucl Engn, Cambridge, MA 02139 USAMIT, Dept Nucl Engn, Cambridge, MA 02139 USA
Cory, DG
[1
]
机构:
[1] MIT, Dept Nucl Engn, Cambridge, MA 02139 USA
[2] Los Alamos Natl Lab, Div Theoret Phys, Los Alamos, NM 87455 USA
[3] Harvard Univ, Sch Med, BCMP, Boston, MA 02115 USA
来源:
PHYSICAL REVIEW A
|
2000年
/
61卷
/
01期
关键词:
D O I:
10.1103/PhysRevA.61.012302
中图分类号:
O43 [光学];
学科分类号:
070207 ;
0803 ;
摘要:
Extensions of average Hamiltonian theory to quantum computation permit the design of arbitrary Hamiltonians, allowing rotations throughout a large Hilbert space. In this way, the kinematics and dynamics of any quantum system may be simulated by a quantum computer. A basis mapping between the systems dictates the average Hamiltonian in the quantum computer needed to implement the desired Hamiltonian in the simulated system. The flexibility of the procedure is illustrated with NMR on C-13 labeled alanine by creating the nonphysical Hamiltonian sigma(z)sigma(z)sigma(z) corresponding to a three-body interaction.