### Table 1: Results on the spin-glass system with n = 121.

2001

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### Table 3.8: System spin, spilling parameter and Mulliken populations for spin dependent calculations of diatomic molecules.

### Table 2. Spin model-checking result for an elevator system

2006

"... In PAGE 13: ... On the other hand, model-checking pair-wise was achieved up to N = 100 without experiencing exponential blow up. In the verification results ( Table2 ), number of transitions is the number of transitions explored in the search. This is indicative of the amount of work performed in model-checking the given properties, for the given value of N.... ..."

Cited by 1

### Table 3 Summary of results of AutoLink on test and experimental data sets Molecule (BMRB accession number) Number of residues Number of assignable spin systems Number of assigned

"... In PAGE 16: ... Even for data set 6128, which has a high de- gree of overlap, 99% of the correct assignments was achieved. See Table3 for a summary of these tests. 4.... ..."

Cited by 1

### Table 1 Sources of error. Typical reservoir interaction Hamiltonians for a spin-12 system are given. Error Hamiltonian Qubit transform

### Table 1. Comparison of standard Spin against Spin with the proposed compression

"... In PAGE 8: ...slide) were collected from the Internet 1 . Table1 shows the memory required (in Mbytes) followed by the time needed to complete eachvalidation run (in seconds) 2 . The rst column (marked Spin) gives the results for the standard Spin system.... ..."

### Table 1. Comparison of standard Spin against Spin with the proposed compression technique (Spin-C)

"... In PAGE 8: ...and slide) were collected from the Internet2. Table1 shows the memory required (in Mbytes) followed by the time needed to complete each validation run (in seconds)3. The rst column (marked Spin) gives the results for the standard Spin system.... ..."

### Table 5.2: Calculated ground state spins and charges, spin equilibrium constants (Kspin) and high-spin fractions for P450 systems studied. In some cases multiple values have been reported for the spin equilibrium constants resulting in a range of possible HS fractions. No spin equilibrium data was available for the metyrapone-bound system.

### Table 2: Table of coe cients of the seven diagonal product oper- ators corresponding to each basic pseudo-spinor for a three-spin system. The spectra that are expected from each of these sums, af- ter appropriate one-spin readout pulses, can be worked out in a straightforward fashion, and the experiments needed to validate this, as well as the usual Pound-Overhauser, implementation of the To oli gate are underway.

in Nuclear Magnetic Resonance Spectroscopy: An Experimentally Accessible Paradigm for Quantum Computing

"... In PAGE 5: ... The matrix of the above To oli pulse sequence is easily shown to be ?1 p2 times: 0 B B B B B B B B B B @ 1 + i 0 0 0 0 0 0 0 0 1 ? i 0 0 0 0 0 0 0 0 i 0 0 0 0 0 0 0 0 ?i 0 0 0 0 0 0 0 0 i 0 0 0 0 0 0 0 0 ?i 0 0 0 0 0 0 0 0 0 1 ? i 0 0 0 0 0 0 ?1 ? i 0 1 C C C C C C C C C C A (22) Hence the output of the gate is in the third bit; the output could easily have been placed in the rst or second bit by applying the =2 pulses to the corresponding spin. Once again, the e ect of the To oli sequence on the ac- tual NMR spectra (after one-spin \readout quot; pulses) of the eight basic pseudo-pure states is most easily established by determining how it a ects the seven diagonal product op- erators (see Table2 ). Unlike the XOR sequence, however, the To oli sequence does not simply permute these prod- uct operators; instead, it results in a sum of such diagonal operators, e.... ..."

### TABLE 1: Ground-State and Excitation Energies of the Different Pt-Clusters with Their Corresponding Spins. Listed Are All Excitation Energies of Spin-States near That of the Ground-State System

2003

Cited by 1