Influence of a new energy scale on conductance fluctuations and weak localization in ultrasmall metallic nanobridges

1993 ◽  
Vol 70 (6) ◽  
pp. 841-844 ◽  
Author(s):  
U. Murek ◽  
R. Schäfer ◽  
W. Langheinrich
2010 ◽  
Vol 19 (14) ◽  
pp. 2325-2330
Author(s):  
SOURISH DUTTA ◽  
ROBERT J. SCHERRER ◽  
STEPHEN D. H. HSU

We propose a class of simple dark energy models which predict a late-time dark radiation component and a distinctive time-dependent equation of state w(z) for redshift z < 3. The dark energy field can be coupled strongly enough to standard model particles to be detected in colliders, and the model requires only modest additional particle content and little or no fine-tuning other than a new energy scale of order milli-electron volts.


2014 ◽  
Vol 568 (5) ◽  
pp. 052028 ◽  
Author(s):  
Alejandro Ferrón ◽  
Daniel Domínguez ◽  
María José Sánchez

2002 ◽  
Vol 71 (12) ◽  
pp. 2832-2835 ◽  
Author(s):  
Naoki Momono ◽  
Toshiaki Matsuzaki ◽  
Migaku Oda ◽  
Masayuki Ido

1993 ◽  
Vol 48 (20) ◽  
pp. 15218-15236 ◽  
Author(s):  
Daniel Loss ◽  
Herbert Schoeller ◽  
Paul M. Goldbart

2003 ◽  
Vol 17 (18n20) ◽  
pp. 3225-3230
Author(s):  
Han-Yong Choi ◽  
Jung-Woo Yoo

The marginal Fermi liquid (MFL) which describes the anomalous normal state of the cuprates is extended to a d-wave superconductive state. A phenomenological collective excitation, P0(ω,T), is taken such that it gives rise to, after renormalization, the MFL behavior in the normal state. With the P0, the renormalized excitation spectrum and pairing function in superconductive state are calculated self-consistently within the Eliashberg formalism. In the superconductive state, the self-energy deviates from the normal state MFL ω/T-scaling and develops a new energy scale of ω0≈2Δ, where Δ is the pairing amplitude.


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