Spin and charge necklaces at commensurate filling
نویسندگان
چکیده
منابع مشابه
Inhomogeneous CuO6 tilt distribution and charge-spin correlations in La2-x-yNdySrxCuO4 around the commensurate hole concentration
A. Gozar,* B. S. Dennis, T. Siegrist, Y. Horibe, G. Blumberg, Seiki Komiya, and Yoichi Ando Bell Laboratories, Lucent Technologies, Murray Hill, New Jersey 07974, USA University of Illinois at Urbana-Champaign, Illinois 61801-3080, USA Rutgers University, Piscataway, New Jersey 08854, USA Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan ~Received 21 May 2003; ...
متن کاملGeons with spin and charge
We construct new geon-type black holes in D ≥ 4 dimensions for Einstein’s theory coupled to gauge fields. A static nondegenerate vacuum black hole has a geon quotient provided the spatial section admits a suitable discrete isometry, and an antisymmetric tensor field of rank 2 or D − 2 with a pure F 2 action can be included by an appropriate (and in most cases nontrivial) choice of the field str...
متن کاملCharge, Spin and Momentum Density
C427 of the complexes has been investigated by theoretical calculations[2], but is still in controversy. Here we show the bonding nature of the 1zirconacyclopent-3-yne complex by means of experimental charge density analysis. Diffraction data were collected using synchrotron radiations at KEK PF-AR NW2 beam line by Rigaku Mercury CCD diffractometer up to sin / = 1.0 Å. Multipole expansion metho...
متن کاملCharge, Spin and Momentum Density
A six-coordinated iron(II) complex, t-Fe(tzpy)2(NCS)2 (tzpy = 3(2-pyridyl)[1,2,3]triazolo[1,5-a]pyridine), undergoes a graduate spin transition from a paramagnetic high spin state (T2, S = 2, HS-1) above 200K to a diamagnetic low spin state (A1, S = 0, LS-1) below 75 K according to the magnetic measurement. The crystal structures of both HS-1 and LS-1 are studied at 298 and 40K respectively. Si...
متن کاملNecklaces , Convolutions , and X +
We give subquadratic algorithms that, given two necklaces each with n beads at arbitrary positions, compute the optimal rotation of the necklaces to best align the beads. Here alignment is measured according to the `p norm of the vector of distances between pairs of beads from opposite necklaces in the best perfect matching. We show surprisingly different results for p = 1, p = 2, and p =∞. For...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
ژورنال
عنوان ژورنال: Journal of Physics: Conference Series
سال: 2009
ISSN: 1742-6588,1742-6596
DOI: 10.1088/1742-6596/150/4/042092