Particle in a box with a δ-function potential: Strong and weak coupling limits

Mesoscopic Anderson box: Connecting weak to strong coupling

Dong E. Liu,1,* Sébastien Burdin,2,3 Harold U. Baranger,1 and Denis Ullmo4,5,† 1Department of Physics, Duke University, Box 90305, Durham, North Carolina 27708-0305, USA 2Univ Bordeaux, LOMA, UMR 5798, F-33400 Talence, France, EU 3CNRS, LOMA, UMR 5798, F-33400 Talence, France, EU 4Univ Paris-Sud, LPTMS, UMR8626, F-91405 Orsay, France, EU 5CNRS, F-91405 Orsay, France, EU (Received 3 February 201...

On Box, Weak Box and Strong Compactness

One of the most important goals of set theorists over the last few years has been to re-prove old results which previously had used very strong assumptions from hypotheses which, at least prima facie, are weaker. Examples of these abound, including, but certainly not limited to, the work of Woodin and Cummings (see [3]) on the Singular Cardinals Problem, in which results previously obtained by ...

a generalization of strong causality

در این رساله t_n - علیت قوی تعریف می شود. این رده ها در جدول علیت فضا- زمان بین علیت پایدار و علیت قوی قرار دارند. یک قضیه برای رده بندی آنها ثابت می شود و t_n- علیت قوی با رده های علی کارتر مقایسه می شود. همچنین ثابت می شود که علیت فشرده پایدار از t_n - علیت قوی نتیجه می شود. بعلاوه به بررسی رابطه نظریه دامنه ها با نسبیت عام می پردازیم و ثابت می کنیم که نوع خاصی از فضا- زمان های علی پایدار, ب...

The Pomeron in the weak and strong coupling limits and kinematical constraints

We show that a resummation model for the evolution kernel at small x creates a bridge between the weak and strong couplings. The resummation model embodies DGLAP and BFKL anomalous dimensions at leading logarithmic orders, as well as a kinematical constraint on the real emission part of the kernel. In the case of pure gluodynamics the strong coupling limit of the Pomeron intercept is consistent...

Weak coupling limits in a stochastic model of heat conduction