Generation of Fock states in a superconducting quantum circuit

被引:449
作者
Hofheinz, Max [1 ]
Weig, E. M. [1 ]
Ansmann, M. [1 ]
Bialczak, Radoslaw C. [1 ]
Lucero, Erik [1 ]
Neeley, M. [1 ]
O'Connell, A. D. [1 ]
Wang, H. [1 ]
Martinis, John M. [1 ]
Cleland, A. N. [1 ]
机构
[1] Univ Calif Santa Barbara, Dept Phys, Santa Barbara, CA 93106 USA
基金
美国国家科学基金会;
关键词
D O I
10.1038/nature07136
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
Spin systems and harmonic oscillators comprise two archetypes in quantum mechanics(1). The spin-1/2 system, with two quantum energy levels, is essentially the most nonlinear system found in nature, whereas the harmonic oscillator represents the most linear, with an infinite number of evenly spaced quantum levels. A significant difference between these systems is that a two- level spin can be prepared in an arbitrary quantum state using classical excitations, whereas classical excitations applied to an oscillator generate a coherent state, nearly indistinguishable from a classical state(2). Quantum behaviour in an oscillator is most obvious in Fock states, which are states with specific numbers of energy quanta, but such states are hard to create(3-7). Here we demonstrate the controlled generation of multi- photon Fock states in a solid- state system. We use a superconducting phase qubit(8), which is a close approximation to a two- level spin system, coupled to a microwave resonator, which acts as a harmonic oscillator, to prepare and analyse pure Fock states with up to six photons. We contrast the Fock states with coherent states generated using classical pulses applied directly to the resonator.
引用
收藏
页码:310 / 314
页数:5
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