Obtaining T 1 - T 2 distribution functions from 1-dimensional T 1 and T 2 measurements: The pseudo 2-D relaxation model

Time T 0 T 1 T 2 T 3 ………. T N the Argument from Relativity

Professor JeeLoo Liu Our common assumptions: 1. Things persist through time. 2. The familiar objects and persons with which we interact on a regular basis persist from day to day. 3. We ourselves are the same person as the one who existed yesterday and the day before.... The issue: What is it for a thing to persist through time? ___ Two theories: [A]. strict identity (one and the same thing) of...

1 5 D ec 1 99 8 Magnetic and Charge Correlations of the 2 - dimensional t − t ′ − U Hubbard model

Using a spin-rotation invariant six-slave boson representation, we study the square lattice Hubbard model with nearest-neighbor hopping t and next-nearest neighbor hopping t ′. We discuss the influence of t ′ on the charge and magnetic properties. In the hole-doped domain, we find that a negative t ′ strongly favors itinerant ferromag-netism over any incommensurate phase, especially in the stro...

Generalized CP 1 model from t 1 − t 2 − J model

A long-wavelength, low-frequency effective theory is obtained from t1− t2−J model. The action is written in terms of two-component bose spinor fields (CP 1 fields) and two spinless Fermi fields. The generalized CP 1 model is invariant under U(1) gauge transformations. The bose fields and one of the Fermi fields have charge +1 while the other Fermi field has charge −1 with respect to these trans...

Age CN T 1 CN T 2 Ca4227 T

Table A1: At high resolution (∼ 0.3 ˚ A), T98 indices of BSPs obtained with the fitting functions (FFs) method.

The Homology of Sl 2 (f T; T ?1 ])