Ph.D. Thesis - Physics

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This is the script that calls the above function, used for studying the effective J value as a function of the gradient in the state-dependent force. % ising_small_rs_script.m % Rob Clark % 27 March 2009 clear; close all; J = 1e3; B = -J; A = 0.1; grads = linspace(0,1,10); % Gradient is relative to A. for ii = 1:length(grads) % Calculate average J for a given grad Jav = J; [Jm(ii),bigerrs(ii)] = ising_small_rs_fn(J,Jav,A,grads(ii)); % Calculate error with new average J [Jcr,smallerrs(ii)] = ising_small_rs_fn(J,Jm(ii),A,grads(ii)); end figure(101); plot(grads,Jm,’ro’); xlabel(’Force gradient’); ylabel(’J_{av}’); figure(102); plot(grads,bigerrs,’ro’); xlabel(’Force gradient’); ylabel(’Uncorrected error’); figure(103); plot(grads,smallerrs,’ro’); xlabel(’Force gradient’); ylabel(’Corrected error’); 234
A.3 Simulation with constant force in space and linear variation in time % File: ising_small_tdep.m % Author: Rob Clark % Simulates Ising model with and without micromotion, % beginning with a random two-qubit state. % The state-dependent force increases linearly in time. % Basis generated by {spin space of ion 1} \otimes {spin space of ion 2} % STAGE 1: simple calculation, ising, no vibration clear; close all; % J = 1.000e3; J = 1000; %*343.6/333.34; B = -J; A = .1; Omega = 1.0e6; t = 0:1/(2*Omega):10/J; Fr1 = t/max(t); tstep = t(2)-t(1); sx = [0 1; 1 0]; sz = [1 0; 0 -1]; sztot1 = kron(eye([2 2]),sz) + kron(sz,eye([2 2])); H1 = J*kron(sz,sz) + B*(kron(eye([2 2]), sx) + kron(sx,eye([2 2]))); % Randomize initial state amps = [rand(1),rand(1),rand(1),rand(1)] + i*[rand(1),rand(1),rand(1),rand(1)]; init1 = amps/norm(amps); init1 = init1’; % init1 = [1;0;0;0]; curr = init1; expsz1 = [init1’*sztot1*init1]; for k = 2:length(t) H1 = Fr1(k)^2*J*kron(sz,sz) + B*(kron(eye([2 2]), sx) + kron(sx,eye([2 2]))); curr = expm(-i*H1*tstep)*curr; expsz1 = [expsz1 curr’*sztot1*curr]; end figure(1); hold on; subplot(3,1,1); 235
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An Investigation of Precision and S
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Acknowledgments What a long, strang
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should totally start a band. I also
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2.4 Conclusions and further questio
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7.6.1 Regular array of stationary q
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List of Figures 2-1 The CNOT gate i
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7-12 Magnetic fields due to a “tr
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Chapter 1 Introduction The growth o
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1.1 Quantum information The concept
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us whether the target system obeys
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Nevertheless, there are a number of
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Digital Analog Classical Quantum Sp
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electrodes [TKK + 99]. This heating
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Digital Analog Classical Quantum Sp
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2. Initialization to a simple fiduc
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qubits, and in Ref. [SGA + 05] in t
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the lattice architecture, we discov
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1.6 Contributions to this work In t
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5) Ref. [DLC + 09b] Wiring up trapp
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Chapter 2 Quantum simulation using
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µN the nuclear magneton, and B0 th
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⎡ ⎤ a 0 0 0 ⎢ ⎥ ⎢ ρ2 =
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The same effect as number 2 above i
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where V0 is the maximum signal stre
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actions that occur between nuclei i
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Figure 2-2: The 2,3-dibromothiophen
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detail how this was done with a sim
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and thus requires invocation of the
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Renormalization Group (DMRG), with
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3.3 The bounds on precision In this
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Figure 3-1: A schematic of a generi
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Figure 3-3: The 11.7 T, 500 MHz sup
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. Figure 3-4: The above probe is a
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Figure 3-5: The CHFBr2 molecule. Al
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Figure 3-6: Frequency-domain spectr
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used to extract the answer is irrel
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Chapter 4 Theory and history of qua
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GND RF r ENDCAP 0 z 0 ENDCAP Ring T
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where Q is the charge of the trappe
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angular momentum along the quantiza
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emission from the excited state |
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selection rule ∆m = ±1 is applie
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Figure 4-3: Schematic diagram of sp
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to address an ion in state |↑〉
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the vibrational temperature is low.
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to the design of the trap itself. M
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to the quantum-mechanical ground st
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Chapter 5 Lattice ion traps for qua
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Figure 5-1: Schematic of the lattic
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Figure 5-3: Fit to Eq. 5.2 of the C
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Figure 5-4: The vacuum chamber for
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weeks. Low pressures depend on choo
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Figure 5-5: Left: Level diagram for
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Figure 5-7: (a) Schematic of the cr
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(a) Lattice Trap Schematic TOP PLAT
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mix the microspheres evenly in the
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Using the expression for ωˆr deri
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Figure 5-15: Plot of the motional c
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Figure 5-17: Dependence of the trap
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Chapter 6 Surface-electrode PCB ion
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Figure 6-1: Schematic of a linear i
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Figure 6-2: Layout of the trap elec
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Figure 6-3: Above are the cross sec
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Figure 6-6: Photograph of the trap
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Figure 6-8: CCD image of a cloud of
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Figure 6-9: Measurement results sho
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Figure 6-11: Bastille mounted in th
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Figure 6-13: A diagram of the setup
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Figure 6-14: A plot of the trapped
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allows us to upper-bound the amount
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Chapter 7 Quantum simulation in sur
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Figure 7-1: Left: Uraniborg 1, as r
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Figure 7-3: Calculated secular freq
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Figure 7-5: Left: Structure of 2-D
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Figure 7-7: Scaling of the order of
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involved. Because ions near the cen
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Results Before presenting the numer
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Figure 7-10: Calculation results fo
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7.3 Magnetic gradient forces Now th
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Figure 7-13: Scaling of the J-coupl
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how are single-ion operations to be
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250 psi, which increases to around
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Figure 7-18: At the center of this
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Figure 7-19: The plastic socket tha
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Figure 7-21: The two internal lense
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Figure 7-22: Measured secular frequ
Page 183 and 184: Along ˆy, the spacing is dˆy = 28
Page 185 and 186: of O2 to 2 × 10 −12 torr. Decohe
Page 187 and 188: Part III Toward ion-ion coupling ov
Page 189 and 190: Chapter 8 Motivation for and theory
Page 191 and 192: Figure 8-1: Schematic of the experi
Page 193 and 194: are in close agreement in the case
Page 195 and 196: 8.2.3 Simulated coupling rates We n
Page 197 and 198: Johnson noise We begin our discussi
Page 199 and 200: should suffice. Note that the above
Page 201 and 202: Chapter 9 Measuring the interaction
Page 203 and 204: Figure 9-2: Left: Level diagram for
Page 205 and 206: Figure 9-5: Photograph of the micro
Page 207 and 208: A fit of the resulting curve return
Page 209 and 210: Figure 9-9: Linear fit of the ωˆy
Page 211 and 212: Figure 9-12: Heating rate as determ
Page 213 and 214: Chapter 10 Conclusions and outlook
Page 215 and 216: traps, linking ions using photons,
Page 217 and 218: Bibliography [ADM05] Paul M. Alsing
Page 219 and 220: [CGB + 94] J. I. Cirac, L. J. Garay
Page 221 and 222: [GME + 02] M. Greiner, O. Mandel, T
Page 223 and 224: [LCL + 07] D. R. Leibrandt, R. J. C
Page 225 and 226: [PC04a] D. Porras and J. I. Cirac.
Page 227 and 228: [TBZ05] L. Tian, R. Blatt, and P. Z
Page 229 and 230: Appendix A Matlab code for Ising mo
Page 231 and 232: err_result = mean(theerr) 231
Page 233: J = J0; Jt(1) = J; Bt(1) = B; for k
Page 237 and 238: Appendix B Mathematica code for ion
Page 239 and 240: 2 crystal_shape_6uraniborg.nb Out[6
Page 241 and 242: Appendix C How to trap ions in a cl
Page 243 and 244: Finally, we note that the chilled w
Page 245 and 246: C.4 Laser alignment and imaging As
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