Repository to store the basic code of trapped ion via qutip(https://github.com/qutip)
Deduce the final probability of excited state after a Ramsey sequence as followed slides from zihan's JC
- What kind of noise can be eliminated by spin echo?
- In the addressing error model, compare the error correction effect of composite pulse sequences SK1, N2, B2 for different values of base errors
- In the amplitude error model, compare the error correction effect of composite pulse sequences SK1, N2, B2 for different values of base errors
Based on AE scheme,calculate the waveform of adiabatic passage with CD-drive Hamiltonian
Derive the effective results to drive two-photon Raman transitions and use the Qutip to calculate the time-evolution of the raman transition with/without deca
We will now investigate the generation and characterizing of nonclassical motional states in a trapped ion system as described by [Meekhof et al. in PhysRevLett. 76.1796 (1996).] The authors generate the thermal, Fock, coherent, and squeezed state of motional of a single Be+ ion. Then they detect the state of atomic motion by observing the evolution of the atom’s internal levels under the influence of a JCM-type interaction.
Reproduce the four population plots of four different motional states in this reference as closely as possible and learn how they generate these states.
We can also just apply a multi-frequency laser field, with each frequency component resonant with one of the transitions to generate the coherent state and squeezing state.[ Kienzler D, Lo H Y, Keitch B, et al. Science, 2015, 347(6217): 53-56.]
Reproduce the Figure 2 to learn the technology of how to generate the coherent state and squeezing state by simultaneously apply the multi-frequency laser field.
Rabi oscillation
- Use Qutip to calculate the Rabi oscillation under a perfect drive, plot the following graphs (with the correct labels): 1. population evolution with time; 2. Fixed time, population vs. scanning frequency; 3. Evolution on the Bloch sphere.
- Suppose we have 20% and 50% amplitude error, respectively, re-plot the evolution on the Bloch sphere
- Plot the spin evolution under a perfect Ramsey experiment
- Suppose during the free evolution, we have random phase shifts that varies from shot to shot, but is fixed in a single experiment (for example caused by slowly changing magnetic field for a Zeeman sensitive qubit). Take a uniform distribution between [0, π/6] and average over 100 shots, how much does the Ramsey contrast decay?
- Numerically simulate how spin echo can remove this (although very ideal) perturbation. Show it on the Bloch sphere.
Composite pulse sequence vs. Counter diabetic driving
- Take an SK1 pulse sequence for example, and we want to flip the qubit from up to down. Calculate the qubit evolution with SK1 sequence and CD drive (e.g. Alberly-Elden scheme mentioned in our journal club), plot them on the bloch sphere.
- Suppose we have 20% and 50% amplitude error, respectively, re-plot the evolution on the Bloch sphere.
We will now investigate EIT cooling as described by Morigi et. al. in Phys. Rev. Lett. 85, 4458 (2000). This paper is also available at arxiv.org/abs/quant-ph/0005009.
Reproduce the plot in Fig. 3 of this reference as closely as possible. You do not have to reproduce the inset. Reproduce both their Monte-Carlo result (instead using our master equation approach) as well as the rate equation result described in the paper. You may assume that the spontaneous emission is equally likely to cause decay into either ground state. This simulation will also take some time to run, this time due to the relatively large Hilbert space necessary to describe the problem. If it takes too long, feel free to reduce the initial number of motional quanta in order to reduce the size of the Hilbert space.
Hint 1: Make sure to start with a thermal state as the initial motional state.
Hint 2: Pay specific attention to the Lamb-Dicke parameters!
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Derive the effective results to drive two-photon Raman transitions.
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Write code to verify that the adiabatic elimination procedure is valid, assuming we start in the |0⟩ state
We will now investigate the generation and characterizing of nonclassical motional states in a trapped ion system as described by Meekhof et al. in PhysRevLett. 76.1796 (1996). The authors generate the thermal, Fock, coherent, and squeezed state of motional of a single Be+ ion. Then they detect the state of atomic motion by observing the evolution of the atom’s internal levels under the influence of a JCM-type interaction.
Reproduce the four population plots of four different motional states in this reference as closely as possible.