Meijer G-function

Results: 53



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21The Performance of a New Hybrid Classifier Based on Boxes and Nearest Neighbors Martin Anthony Joel Ratsaby

The Performance of a New Hybrid Classifier Based on Boxes and Nearest Neighbors Martin Anthony Joel Ratsaby

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Source URL: www.cs.uic.edu

Language: English - Date: 2013-08-09 14:57:11
22Theory and Applications of Categories, Vol. 28, No. 23, 2013, pp. 733–779. THE ALGEBRA OF THE NERVES OF OMEGA-CATEGORIES RICHARD STEINER Abstract. We show that the nerve of a strict omega-category can be described alg

Theory and Applications of Categories, Vol. 28, No. 23, 2013, pp. 733–779. THE ALGEBRA OF THE NERVES OF OMEGA-CATEGORIES RICHARD STEINER Abstract. We show that the nerve of a strict omega-category can be described alg

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Source URL: www.emis.de

Language: English - Date: 2013-09-01 12:03:00
23Kernel Choice and Classifiability for RKHS Embeddings of Probability Distributions Bharath K. Sriperumbudur Department of ECE UC San Diego, La Jolla, USA

Kernel Choice and Classifiability for RKHS Embeddings of Probability Distributions Bharath K. Sriperumbudur Department of ECE UC San Diego, La Jolla, USA

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Source URL: www.select.cs.cmu.edu

Language: English - Date: 2009-11-08 23:50:48
24Dynamic Systems and Applications[removed]394 IMPROVEMENTS OF COMPOSITION RULE FOR THE CANAVATI FRACTIONAL DERIVATIVES AND APPLICATIONS TO OPIAL-TYPE INEQUALITIES ´ J. PECARI

Dynamic Systems and Applications[removed]394 IMPROVEMENTS OF COMPOSITION RULE FOR THE CANAVATI FRACTIONAL DERIVATIVES AND APPLICATIONS TO OPIAL-TYPE INEQUALITIES ´ J. PECARI

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Source URL: bib.irb.hr

Language: English - Date: 2011-11-16 05:47:22
25Report no[removed]Computing Aα, log(A) and related matrix functions by contour integrals Nicholas Hale Oxford University Computing Laboratory

Report no[removed]Computing Aα, log(A) and related matrix functions by contour integrals Nicholas Hale Oxford University Computing Laboratory

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Source URL: eprints.maths.ox.ac.uk

Language: English - Date: 2011-05-06 06:09:08
26

PDF Document

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Source URL: cs.uwaterloo.ca

Language: English - Date: 2011-11-21 10:47:28
27Preprint ANL/MCS[removed]CONVERGENCE OF A CLASS OF SEMI-IMPLICIT TIME-STEPPING SCHEMES FOR NONSMOOTH RIGID MULTIBODY DYNAMICS BOGDAN I. GAVREA∗ , MIHAI ANITESCU† , AND FLORIAN A. POTRA‡ Abstract. In this work we

Preprint ANL/MCS[removed]CONVERGENCE OF A CLASS OF SEMI-IMPLICIT TIME-STEPPING SCHEMES FOR NONSMOOTH RIGID MULTIBODY DYNAMICS BOGDAN I. GAVREA∗ , MIHAI ANITESCU† , AND FLORIAN A. POTRA‡ Abstract. In this work we

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Source URL: www.math.umbc.edu

Language: English - Date: 2006-12-01 09:40:41
28Week 6 (due Nov. 13) Reading: Srednicki, sections 6 and[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q 0 , q; T ) = hq 0 |e−iHT |qi. Here H is the usual Hamiltonian, i.e.

Week 6 (due Nov. 13) Reading: Srednicki, sections 6 and[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q 0 , q; T ) = hq 0 |e−iHT |qi. Here H is the usual Hamiltonian, i.e.

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Source URL: www.theory.caltech.edu

Language: English - Date: 2009-11-07 12:59:11
29Week 5 (due Nov. 7) Reading: Srednicki, sections 6 and[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q ′ , q; T ) = hq ′ |e−iHT |qi. Here H is the usual Hamiltonian, i.e.

Week 5 (due Nov. 7) Reading: Srednicki, sections 6 and[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q ′ , q; T ) = hq ′ |e−iHT |qi. Here H is the usual Hamiltonian, i.e.

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Source URL: www.theory.caltech.edu

Language: English - Date: 2007-11-02 00:50:25
30Week 4 (due Oct[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q 0 , q; T ) = hq 0 |e−iHT |qi. Here H is the usual Hamiltonian, i.e. H=

Week 4 (due Oct[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q 0 , q; T ) = hq 0 |e−iHT |qi. Here H is the usual Hamiltonian, i.e. H=

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Source URL: www.theory.caltech.edu

Language: English - Date: 2013-10-24 00:38:18