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  <item rdf:about="http://hdl.handle.net/2440/53618">
    <title>Interplay of spin and orbital angular momentum in the proton</title>
    <link>http://hdl.handle.net/2440/53618</link>
    <description>Title: Interplay of spin and orbital angular momentum in the proton
&lt;br/&gt;
&lt;br/&gt;Author: Thomas, Anthony William
&lt;br/&gt;
&lt;br/&gt;Description: ©2008 The American Physical Society</description>
  </item>
  <item rdf:about="http://hdl.handle.net/2440/53584">
    <title>The enantiomer of octreotate binds to all five somatostatin receptors with almost equal micromolar affinity - A comparison with Sandostatin®.</title>
    <link>http://hdl.handle.net/2440/53584</link>
    <description>Title: The enantiomer of octreotate binds to all five somatostatin receptors with almost equal micromolar affinity - A comparison with Sandostatin®.
&lt;br/&gt;
&lt;br/&gt;Author: Gardiner, James; Langenegger, Daniel; Hoyer, Daniel; Beck, Albert K.; Mathad, R. I.; Seebach, Dieter
&lt;br/&gt;
&lt;br/&gt;Abstract: Octreotate (1b) is the octreotide (SANDOSTATIN®; 1a) analogue, carrying a C-terminal CO2H (Thr) instead of the CH2OH (threoninol) group. In pursuit of our interest in unnatural peptides, we have now synthesized (by the solid-phase Fmoc method) the enantiomeric form 2 of octreotate and determined its affinity for the five human somatostatin (SRIF) receptors (hsst1-5). The binding was found to be 9.1, 4.1, 1.0, 1.4, and 4.2 M, respectively. This almost equal one-digit micromolar affinity of ent-octreotate (2) to all five receptors contrasts with the behavior of most other somatostatin mimics including SANDOSTATIN® (octreotide; 1a) and [Tyr3]-octreotate (1c), which have affinities for the various receptors differing up to and above 104-fold. Thus, the structure of the new compound does not prevent binding, albeit more weakly than its pseudo-enantiomer octreotide, and there is hardly any selectivity of the peptide-protein interaction (PPI) for any one of the five SRIF G-protein coupled receptors (GPCRs). Since the detailed structure(s) of these membrane-embedded receptors is unknown (no X-ray structure!), the result described here may be useful for modeling structures by comparing the affinities of the numerous known somatostatin mimics.</description>
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  <item rdf:about="http://hdl.handle.net/2440/53550">
    <title>The Strong-coupling limit of minimal lattace landau gauge</title>
    <link>http://hdl.handle.net/2440/53550</link>
    <description>Title: The Strong-coupling limit of minimal lattace landau gauge
&lt;br/&gt;
&lt;br/&gt;Author: Sternbeck, Andre; Von Smekal, Lorenz Johann Maria
&lt;br/&gt;
&lt;br/&gt;Description: Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence.; Submitted to Cornell University’s online archive www.arXiv.org in 2008 by Andre Sternbeck.</description>
  </item>
  <item rdf:about="http://hdl.handle.net/2440/53549">
    <title>Lattice Landau Gauge via Stereographic Projection</title>
    <link>http://hdl.handle.net/2440/53549</link>
    <description>Title: Lattice Landau Gauge via Stereographic Projection
&lt;br/&gt;
&lt;br/&gt;Author: Von Smekal, Lorenz Johann Maria; Jorkowski, Alexander Felix; Mehta, Dhagash Bharatbhai; Sternbeck, Andre
&lt;br/&gt;
&lt;br/&gt;Abstract: The complete cancellation of Gribov copies and the Neuberger 0=0 problem of lattice BRST can&#xD;
be avoided in modified lattice Landau gauge. In compact U(1), where the problem is a lattice&#xD;
artifact, there remain to be Gribov copies but their number is exponentially reduced. Moreover,&#xD;
there is no cancellation of copies there as the sign of the Faddeev-Popov determinant is positive.&#xD;
Applied to the maximal Abelian subgroup this avoids the perfect cancellation amongst the&#xD;
remaining Gribov copies for SU(N) also. In addition, based on a definition of gauge fields on&#xD;
the lattice as stereographically-projected link variables, it provides a framework for gauge fixed&#xD;
Monte-Carlo simulations. This will include all Gribov copies in the spirit of BRST. Their average&#xD;
is not zero, as demonstrated explicitly in simple models. This might resolve present discrepancies&#xD;
between gauge-fixed lattice and continuum studies of QCD Green’s functions.
&lt;br/&gt;
&lt;br/&gt;Description: Copyright © owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence.; Submitted to Cornell University’s online archive www.arXiv.org in 2008 by Lorenz von Smekal.</description>
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