PDF (double-sided) - Physics Department, UCSB - University of ...
PDF (double-sided) - Physics Department, UCSB - University of ... PDF (double-sided) - Physics Department, UCSB - University of ...
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Chapter 10 Hidden Variable Theories versus Quantum Mechanics 10.1 Introduction 10.1.1 Is Quantum Mechanics Incomplete? Due to its radically new way of seeing the world, quantum mechanics was initially met with great skepticism from many renowned physicists, including Albert Einstein. Specifically the idea that the world was inherently non-deterministic and random did not sit well with Einstein and many of his colleagues. This dislike culminated in Einstein’s famous statement: “I, at any rate, am convinced that 225
- Page 202 and 203: 8.1 Squid I/V Response As explained
- Page 204 and 205: a digital signal via the use of a c
- Page 206 and 207: energy landscape (see Chapter 2.2.3
- Page 208 and 209: Figure 8.3: Squid Steps Failure Mod
- Page 210 and 211: At this point, the squid ramp can b
- Page 212 and 213: starts to tunnel to the neighboring
- Page 214 and 215: Figure 8.5: General Bias Sequence -
- Page 216 and 217: Figure 8.7: Spectroscopy - a) Bias
- Page 218 and 219: Figure 8.8: Rabi Oscillation - a) B
- Page 220 and 221: ensemble with respect to each other
- Page 222 and 223: Figure 8.10: T 1 - a) Bias sequence
- Page 224 and 225: Figure 8.11: Ramsey - a) Bias seque
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- Page 228 and 229: photon excitation behaves similarly
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- Page 238 and 239: Figure 9.4: Capacitive Coupling Swa
- Page 240 and 241: Figure 9.6: Capacitive Coupling Pha
- Page 242 and 243: a phase difference of 0 ◦ rather
- Page 244 and 245: Figure 9.7: Fine Spectroscopy of Re
- Page 246 and 247: Figure 9.8: Swapping Photon into Re
- Page 248 and 249: esonator. The latter calibration is
- Page 250 and 251: Figure 9.11: Resonator T 1 - a) Seq
- Page 254 and 255: He does not throw dice” [Einstein
- Page 256 and 257: (independent of which axis it is),
- Page 258 and 259: of E xy is measured by expressing i
- Page 260 and 261: For a measurement of two particles
- Page 262 and 263: 10.2.1 Photons The first and most n
- Page 264 and 265: 10.2.3 Ion and Photon In the attemp
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- Page 268 and 269: 11.1 State Preparation Since the ab
- Page 270 and 271: Figure 11.1: Bell State Preparation
- Page 272 and 273: Table 11.1: Entangled State Density
- Page 274 and 275: Figure 11.2: Bell Measurements - a)
- Page 276 and 277: 11.2.3 Statistical Analysis For the
- Page 278 and 279: 11.3 Calibration The most difficult
- Page 280 and 281: Table 11.4: Sequence Parameters - R
- Page 282 and 283: ally determine an optimal value for
- Page 284 and 285: ages are based on this method, incl
- Page 286 and 287: equires to converge. Since the algo
- Page 288 and 289: Table 11.7: Bell Violation Results
- Page 290 and 291: Table 11.9: Error Budget - Capaciti
- Page 292 and 293: Table 11.10: Bell Violation Results
- Page 294 and 295: Bell inequality. To make this claim
- Page 296 and 297: Table 11.12: Bell Violation Results
- Page 298 and 299: 11.5.2 Dependence of S on Sequence
- Page 300 and 301: point where the measurement happens
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