!"#$%#&'()$*+$&#'',#-*./&*.&$0-1./& 1'2+#"&3,"4$&(*/(,-&0(#.&56 78 &9:+% 7

상대론적고에너지중이온충돌에서 제트입자와관련된제동복사 박가영 인하대학교 윤진희교수님, 권민정교수님

상대론적고에너지중이온충돌에서 제트입자와관련된제동복사 박가영 인하대학교 윤진희교수님, 권민정교수님 Motivation Bremsstrahlung is a major rocess losing energies while jet articles get through the medium. BUT it should be quite different from low energy

ˆŒ œ ƒ ƒ ˆ ˆŸ ˆ Š ˆ 137 Cs Š ˆ Œ.

Ó³ Ÿ. 2017.. 14, º 6(211).. 630Ä636 ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ. Š ˆŒ ˆ Š ˆŸ ˆŸ ˆŒ œ ƒ ƒ ˆ ˆŸ ˆ Š ˆ 137 Cs Š ˆ Œ. œ.., 1,.. ³,. ƒ. Š ² ±μ,.. ³ ±,.. ³ μ,. ˆ. É ²μ,. ˆ. ÕÉÕ ±μ, ƒ.. Ë,, ˆ.. ±μ ˆ É ÉÊÉ μ Ð Ë ± ³.. Œ.

Dong Liu State Key Laboratory of Particle Detection and Electronics University of Science and Technology of China

Dong Liu State Key Laboratory of Particle Detection and Electronics University of Science and Technology of China ISSP, Erice, 7 Outline Introduction of BESIII experiment Motivation of the study Data sample

(1) Describe the process by which mercury atoms become excited in a fluorescent tube (3)

Q1. (a) A fluorescent tube is filled with mercury vapour at low pressure. In order to emit electromagnetic radiation the mercury atoms must first be excited. (i) What is meant by an excited atom? (1) (ii)

Laboratory Studies on the Irradiation of Solid Ethane Analog Ices and Implications to Titan s Chemistry

Laboratory Studies on the Irradiation of Solid Ethane Analog Ices and Implications to Titan s Chemistry 5th Titan Workshop at Kauai, Hawaii April 11-14, 2011 Seol Kim Outer Solar System Model Ices with

P = E /c. p γ = E /c. (p) 2 = (p γ ) 2 + (p ) 2-2 p γ p cosθ E γ. (pc) (E γ ) (E ) 2E γ E cosθ E m c Eγ

Σκέδαση Compton Το φαινόμενο Compton περιγράφει ργρ τη σκέδαση ενός φωτονίου από ένα ελεύθερο ατομικό ηλεκτρόνιο: γ + e γ + e. To φωτόνιο δεν εξαφανίζεται μετά τη σκέδαση αλλά αλλάζει κατεύθυνση και ενέργεια.

1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions

1 Decay Scheme Cf- disintegrates by alpha emissions mainly to the Cm-248 ground state level, and by spontaneous fission for 3,086(8) %. The average number of neutrons emitted by spontaneous fission is:

Coupling of a Jet-Slot Oscillator With the Flow-Supply Duct: Flow-Acoustic Interaction Modeling

1th AIAA/CEAS Aeroacoustics Conference, May 006 interactions Coupling of a Jet-Slot Oscillator With the Flow-Supply Duct: Interaction M. Glesser 1, A. Billon 1, V. Valeau, and A. Sakout 1 mglesser@univ-lr.fr

Questions on Particle Physics

Questions on Particle Physics 1. The following strong interaction has been observed. K + p n + X The K is a strange meson of quark composition u s. The u quark has a charge of +2/3. The d quark has a charge

Ó³ Ÿ , º 4Ä5(174Ä175).. 629Ä634 ˆ ˆŠ ˆ ˆŠ Š ˆ. .. Ëμ μ,.. μ, Š.. ±μ. Î ± É ÉÊÉ ³..., Œμ ±

Ó³ Ÿ. 2012.. 9, º 4Ä5(174Ä175).. 629Ä634 ˆ ˆŠ ˆ ˆŠ Š ˆ Ÿ Œ Ÿ.. Ëμ μ,.. μ, Š.. ±μ Î ± É ÉÊÉ ³..., Œμ ± Ö Ì μ ÊÌ É³μ Ë μ μ ² Ö ³ ± ³ ²Ó μ³ Ö μ³ Êɱ μé 0,8 μ 1,2 Œ É μ μ ³ Ê²Ó μ É μ ±μ ²ÊÎ Ô ± Éμ μ² 5 ±Ô

Wolfgang Sandner Director General and CEO ELI Delivery Consortium International Association (AISBL)

Wolfgang Sandner Director General and CEO ELI Delivery Consortium International Association (AISBL) DESY Zeuthen Seminar, May 12, 2015 Project supported by: initiation parallel implementation joint operation

Σύντομο Βιογραφικό Σημείωμα

Σύντομο Βιογραφικό Σημείωμα Πίνακας επιλεγμένων βιογραφικών στοιχείων Όνομα Θέση στο Έργο Θέση στο Ίδρυμα Προπτυχιακοί τίτλοι σπουδών Μεταπτυχιακοί τίτλοι σπουδών Ειδικές γνώσεις στο γνωστικό αντικείμενο

April MD simulation of interaction between radiation damages and microstructure: voids, helium bubbles and grain boundaries

2137-32 Joint ICTP-IAEA Advanced Workshop on Multi-Scale Modelling for Characterization and Basic Understanding of Radiation Damage Mechanisms in Materials 12-23 April 2010 MD simulation of interaction

Derivation of Optical-Bloch Equations

Appendix C Derivation of Optical-Bloch Equations In this appendix the optical-bloch equations that give the populations and coherences for an idealized three-level Λ system, Fig. 3. on page 47, will be

ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ Ä664

ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ 2017.. 48.. 5.. 653Ä664 ˆ Œ ˆ ˆ e + e K + K nπ (n =1, 2, 3) Š Œ ŠŒ -3 Š - ˆ Œ Š -2000 ƒ.. μéμ Î 1,2, μé ³ ±μ²² μ Í ŠŒ -3: A.. ß ±μ 1,2,. Œ. ʲÓÎ ±μ 1,2,.. ̳ ÉÏ 1,2,.. μ 1,.. ÏÉμ μ 1,.

Ó³ Ÿ , º 6(190) Ä1142. DESY, ƒ ³ Ê, ƒ ³ Ö European XFEL, GmbH, ƒ ³ Ê, ƒ ³ Ö ±Êʳ-,

Ó³ Ÿ. 2014.. 11, º 6(190).. 1134Ä1142 Œ ˆŠ ˆ ˆ Š ƒ Š ˆŒ Š ˆ ˆŸ ŒˆŠ Š œ ˆ Ÿ Š. Ò a,1,. μ ±μ a,. ƒ Íμ a,. ³ÖÉ a,. Ê μ a, Œ. ±μ a,,2, Ÿ. ƒ Õ É,. Õ,3,. μ ±μ,. É,. ²,. Ò,4 a Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê DESY, ƒ ³

CERN-ACC-SLIDES

CERN-ACC-SLIDES-2014-0002 13/05/2014 Francesco.Broggi@mi.infn.it Francesco.Broggi@cern.ch RESMM 14 Wroclaw May13 th 2014 Ti5 Nb 3 Sn cable SimpleGeo Plot 1.0x10 12 Activity Decay After Irradiation LHe

Hours Monday Tuesday Wednesday Thursday Friday. Physics of Diagnostic Radiology. Physics of Diagnostic Radiology. Physics of Diagnostic Radiology

Second Term, Week 1 11 15 January 2010 EXAMS Physiology EXAMS Physiology EXAMS Physiology (16h): G. Panayiotakis, G. Kandarakis Lectures will be given at Computer Lab, 1 st floor, building of the School

Research on mode-locked optical fiber laser

2003 6 20 Research on mode-locked optical fiber laser 1 36303 Abstract- For future ultrahigh-speed optical communications, an ultrashort optical pulse train at a high repetitionrate will be indispensable.

Broadband Spatiotemporal Differential-Operator Representations For Velocity-Dependent Scattering

Broadband Spatiotemporal Differential-Operator Representations For Velocity-Dependent Scattering Dan Censor Ben Gurion University of the Negev Department of Electrical and Computer Engineering Beer Sheva,

P ² ± μ. œ Š ƒ Š Ÿƒ ˆŸ Œ œ Œ ƒˆ. μ²μ μ Œ Ê μ μ ±μ Ë Í μ É Í ±μ ³μ²μ (RUSGRAV-13), Œμ ±, Õ Ó 2008.

P3-2009-104.. ² ± μ ˆ ˆ Š Š ˆ œ Š ƒ Š Ÿƒ ˆŸ Œ œ Œ ƒˆ μ²μ μ Œ Ê μ μ ±μ Ë Í μ É Í ±μ ³μ²μ (RUSGRAV-13), Œμ ±, Õ Ó 2008. ² ± μ.. ²μ μ ± μé±²μ μé ÓÕÉμ μ ±μ μ ±μ ÉÖ μé Ö μ³μðóõ É μ μ ³ ²ÒÌ Ô P3-2009-104 ÓÕÉμ

LIGHT UNFLAVORED MESONS (S = C = B = 0)

LIGHT UNFLAVORED MESONS (S = C = B = 0) For I = 1 (π, b, ρ, a): ud, (uu dd)/ 2, du; for I = 0 (η, η, h, h, ω, φ, f, f ): c 1 (uu + d d) + c 2 (s s) π ± I G (J P ) = 1 (0 ) Mass m = 139.57018 ± 0.00035

1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions

1 Decay Scheme Rh- disintegrates by beta minus emission to the ground state and excited levels of Pd-. Le rhodium se désintègre par émission bêta principalement vers le niveau fondamental et les niveaux

Ó³ Ÿ º 3[120] Particles and Nuclei, Letters No. 3[120]

Ó³ Ÿ. 2004. º 3[120] Particles and Nuclei, Letters. 2004. No. 3[120] Š 621.384.633.5/6 Š ˆ ˆ Šˆ Šˆ Š ˆ Ÿ Ÿ ˆ ˆ.. Œ ϱµ 1,.. µ 1,.. ³ µ 1,. Œ. Ò 1, ƒ.. Ê ±µ 1 Ñ Ò É ÉÊÉ Ö ÒÌ ² µ, Ê Œµ ±µ ± µ Ê É Ò É ÉÊÉ

P Ë ³μ,.. μ μ³μ²μ,.. ŠμÎ μ,.. μ μ,.. Š μ. ˆ œ ˆ Š Œˆ ŠˆŒ ƒ Œ Ÿ ˆŸ Š ˆ ˆ -ˆ ˆŠ

P9-2008-102.. Ë ³μ,.. μ μ³μ²μ,.. ŠμÎ μ,.. μ μ,.. Š μ ˆ œ ˆ Š Œˆ ŠˆŒ ƒ Œ Ÿ ˆŸ Š ˆ ˆ -ˆ ˆŠ Ë ³μ... P9-2008-102 ˆ μ²ó μ Ô± μ³ Î ± ³ μ³ ²Ö μ²êî Ö Êα μ μ - ÉμÎ ± μ²êî É ÒÌ Ê ±μ ÒÌ Êαμ 48 Ö ²Ö É Ö μ μ ±²ÕÎ

ΙΕΥΘΥΝΤΗΣ: Καθηγητής Γ. ΧΡΥΣΟΛΟΥΡΗΣ Ι ΑΚΤΟΡΙΚΗ ΙΑΤΡΙΒΗ

ΠΑΝΕΠΙΣΤΗΜΙΟ ΠΑΤΡΩΝ ΠΟΛΥΤΕΧΝΙΚΗ ΣΧΟΛΗ ΤΜΗΜΑ ΜΗΧΑΝΟΛΟΓΩΝ ΚΑΙ ΑΕΡΟΝΑΥΠΗΓΩΝ ΜΗΧΑΝΙΚΩΝ ΕΡΓΑΣΤΗΡΙΟ ΣΥΣΤΗΜΑΤΩΝ ΠΑΡΑΓΩΓΗΣ & ΑΥΤΟΜΑΤΙΣΜΟΥ / ΥΝΑΜΙΚΗΣ & ΘΕΩΡΙΑΣ ΜΗΧΑΝΩΝ ΙΕΥΘΥΝΤΗΣ: Καθηγητής Γ. ΧΡΥΣΟΛΟΥΡΗΣ Ι ΑΚΤΟΡΙΚΗ

Three coupled amplitudes for the πη, K K and πη channels without data

Three coupled amplitudes for the πη, K K and πη channels without data Robert Kamiński IFJ PAN, Kraków and Łukasz Bibrzycki Pedagogical University, Kraków HaSpect meeting, Kraków, V/VI 216 Present status

6.1. Dirac Equation. Hamiltonian. Dirac Eq.

6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2

Lecture 21: Scattering and FGR

ECE-656: Fall 009 Lecture : Scattering and FGR Professor Mark Lundstrom Electrical and Computer Engineering Purdue University, West Lafayette, IN USA Review: characteristic times τ ( p), (, ) == S p p

X-Y COUPLING GENERATION WITH AC/PULSED SKEW QUADRUPOLE AND ITS APPLICATION

X-Y COUPLING GENERATION WITH AC/PULSED SEW QUADRUPOLE AND ITS APPLICATION # Takeshi Nakamura # Japan Synchrotron Radiation Research Institute / SPring-8 Abstract The new method of x-y coupling generation

Photo-Induced Self-Assembly of Pt(II)-Linked Rings and Cages via the Photolabilization of a Pt(II) Pyridine Bond

Photo-Induced Self-Assembly of Pt(II)-Linked Rings and Cages via the Photolabilization of a Pt(II) Pyridine Bond Ken-ichi Yamashita, Kei-ichi Sato, Masaki Kawano and Makoto Fujita* Contents; Figure S1.

Œ ƒ Š ƒ. .. μéò² ÍÒ 1,2,,.Œ.Šμ²ÓÎÊ ± 3. ƒ Š Œ Š ƒ Ÿ ˆŸ Œ -Š 1813 œ Œ ˆ ˆŸ 1814 ˆ Š ˆ ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ Ä6.

ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ 2014.. 45.. 5Ä6 ˆ ˆ Š Œ ˆ ˆ Œ ƒ Š ƒ Š Œ Š ƒ Ÿ ˆŸ.. μéò² ÍÒ 1,2,,.Œ.Šμ²ÓÎÊ ± 3 1 Í μ ²Ó Ò ² μ É ²Ó ± μ³ ± μ² É Ì Î ± Ê É É, μ³ ±, μ Ö 2 Í μ ²Ó Ò ² μ É ²Ó ± Ö Ò Ê É É Œˆ ˆ, Œμ ± 3 Œμ ±μ

Œ ˆ ˆŸ ˆ Š ˆ ƒ Š Œ Š Š

Ó³ Ÿ. 2012.. 9, º 4Ä5(174Ä175).. 654Ä665 ˆ ˆŠ ˆ ˆŠ Š ˆ Œ ˆ ˆŸ ˆ Š ˆ ƒ Š Œ Š Š.. ÊÉ ±μ,. ˆ. ƒμ μ μ,.. μ Í,.. μ Í,.. μ Í, Š.. É μ,.. Œμ Î ±,.. μ, ƒ.. Ê ±μ,.. ³Êϱ Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê ˆ ±Í μ Ò ±μ³ ² ± ʱ²μÉ

Ó³ Ÿ , º 7(205) Ä1268 ˆ ˆŠ ˆ ˆŠ Š ˆ. ƒ ˆˆ μì Ê ³... Ê ±μ, Œμ ± Í μ ²Ó Ò ² μ É ²Ó ± Ö Ò Ê É É Œˆ ˆ, Œμ ± É ƒ ³³ - μ ª Œμ ±, Œμ ±

Ó³ Ÿ. 2016.. 13, º 7(205).. 1263Ä1268 ˆ ˆŠ ˆ ˆŠ Š ˆ ˆ ˆŸ ˆŸ Œ Š ƒ Š ˆ ƒ Š ˆ Ÿ Œ ƒ ˆ ˆŸ Š Š ˆ œ ˆŸ ˆˆ ƒ.. ƒμ ² Î,1,. Œ. μ²μ μ,.. ² Î,,. ˆ. Š μëμ Éμ,.. Š É ƒ ˆˆ μì Ê ³... Ê ±μ, Œμ ± Í μ ²Ó Ò ² μ É ²Ó ± Ö

Ιατρική Φυσική. Π. Παπαγιάννης Επίκ. Καθηγητής, Εργαστήριο Ιατρικής Φυσικής, Ιατρική Σχολή Αθηνών Γραφείο

Ιατρική Φυσική Π. Παπαγιάννης Επίκ. Καθηγητής, Εργαστήριο Ιατρικής Φυσικής, Ιατρική Σχολή Αθηνών Γραφείο 21 210-746 2442 ppapagi@phys.uoa.gr PHYS215 Ιατρική Φυσική: Δοσιμετρία Ιοντίζουσας Ακτινοβολίας

Advanced operation schemes: two-color, split & delay

Advanced operation schemes: two-color, split & delay Production of two FEL pulses of different wavelengths with a controllable temporal delay (and) Splitting the FEL pulse into two sequential pulses at

P = E /c. p γ = E /c. (p) 2 = (p γ ) 2 + (p ) 2-2 p γ p cosθ E γ. (pc) (E γ ) (E ) 2E γ E cosθ E m c Eγ

Σκέδαση Compton Το φαινόμενο Compton περιγράφει ργρ τη σκέδαση ενός φωτονίου από ένα ελεύθερο ατομικό ηλεκτρόνιο: γ + e γ + e. To φωτόνιο δεν εξαφανίζεται μετά τη σκέδαση αλλά αλλάζει κατεύθυνση και ενέργεια.

PHASE TRANSITIONS IN QED THROUGH THE SCHWINGER DYSON FORMALISM

PHASE TRANSITIONS IN THROUGH THE SCHWINGER DYSON FORMALISM Spyridon Argyropoulos University of Athens Physics Department Division of Nuclear Physics and Elementary Particles Supervisor: C.N. Ktorides Athens

Ó³ Ÿ , º 7(205) Ä1486 ˆ ˆŠ ˆ ˆŠ Š ˆ. . ³ μ 1, ƒ. μ μë,. μ,. ŠÊ² ±μ,. Œ ² μ ± Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê

Ó³ Ÿ. 06.. 3, º 7(05).. 479Ä486 ˆ ˆŠ ˆ ˆŠ Š ˆ Š ˆŒ œ ˆ ˆ - Š Ÿ ˆ Œ Š ƒ ˆŸ. ³ μ, ƒ. μ μë,. μ,. ŠÊ² ±μ,. Œ ² μ ± Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê μ ±É NICA ±²ÕÎ É Ö É ³Ê Ô² ±É μ μ μ μì² Ö Êαμ Ö ÒÌ Î É Í μ μ² μ Ô μ

Lukasz STAWARZ. on Behalf of the Fermi LAT Collaboration.

e-mail: kataoka.jun@waseda.jp 169 8555 3 4 1 739 8526 1 3 1 e-mail: fukazawa@hep01.hep1.hiroshima.u.ac.jp Lukasz STAWARZ 252 5210 3 1 1 e-mail: stawarz@astro.isas.jaxa.jp e-mail: rsato@astro.isas.jaxa.jp

Ó³ Ÿ , º 6(155).. 805Ä813 ˆ ˆŠ ˆ ˆŠ Š ˆ. ˆ.. ³ Ì μ, ƒ.. Š ³ÒÏ, ˆ.. Š Ö. Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê. Ÿ. ʲ ±μ ±

Ó³ Ÿ. 2009.. 6, º 6(155).. 805Ä813 ˆ ˆŠ ˆ ˆŠ Š ˆ Œ ˆ ˆ Œ ˆŒ ˆ ˆ ˆ ˆ ˆ Ÿ Œ ƒ ˆ ˆŠ ˆ.. ³ Ì μ, ƒ.. Š ³ÒÏ, ˆ.. Š Ö Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê Ÿ. ʲ ±μ ± ˆ É ÉÊÉ Ö μ Ë ± μ²ó ±μ ± ³ ʱ, Š ±μ, μ²óï Œ É ³ É Î ±μ ±μ³

Ó³ Ÿ , º 7(205) Ä1403 ˆ ˆŠ ˆ ˆŠ Š ˆ. ˆ É ÉÊÉ ±² μ Ë ±, μ μ μ, μ Ö ² ±É μé Ì Î ± É ÉÊÉ, É ²

Ó³ Ÿ. 2016.. 13, º 7(205).. 1398Ä1403 ˆ ˆŠ ˆ ˆŠ Š ˆ ˆ ˆ Š ˆŸˆ. ˆ. ² ²Ò± a,.. Œ ϱ a, Œ.. μ a,1, ƒ.. Ê ±μ a, ƒ.. ±μ a,.ˆ.ƒ Î,.. Š É,.. μ, ƒ.. ÊÎ,.Š. μé ³±,.. ² μ μ ±,. ƒê a Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê ˆ É ÉÊÉ

Ó³ Ÿ , º 7(163).. 855Ä862 ˆ ˆŠ ˆ ˆŠ Š ˆ. . ƒ. ² ͱ 1,.. μ μ Íμ,.. μ²ö,.. ƒ² μ,.. ² É,.. ³ μ μ, ƒ.. Š ³ÒÏ,.. Œμ μ μ,. Œ.

Ó³ Ÿ. 2010.. 7, º 7(163).. 855Ä862 ˆ ˆŠ ˆ ˆŠ Š ˆ ˆ œ ˆŠ Ÿ ˆŸ Š Ÿ Š. ƒ. ² ͱ 1,.. μ μ Íμ,.. μ²ö,.. ƒ² μ,.. ² É,.. ³ μ μ, ƒ.. Š ³ÒÏ,.. Œμ μ μ,. Œ. Ð ±μ Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê μ Ö ± É μ É Êα Ê ±μ ÒÌ μéμ μ

ΗΛΕΚΤΡΟ-ΟΠΤΙΚΗ & ΕΦΑΡΜΟΓΕΣ

12/10/2016 ΗΛΕΚΤΡΟ-ΟΠΤΙΚΗ & ΕΦΑΡΜΟΓΕΣ Χειμερινό Εξάμηνο 2016-2017 Γενικές Πληροφορίες Ώρα: Πέμπτη 09:00-11:45 Αίθουσα: Αιθ. 103 (Νέα Κτίρια ΗΜΜΥ) Καθηγητής: Ηλίας Ν. Γλύτσης Γραφείο: 2.2.22 Τηλέφωνο: 210-772-2479

ˆŒˆ ˆŸ ˆ Œ ƒ LEPTO/JETSET Ÿ ˆ ƒ

Ó³ Ÿ. 2014.. 11, º 4(188).. 817Ä827 Š Œ œ ƒˆˆ ˆ ˆŠ ˆŒˆ ˆŸ ˆ Œ ƒ LEPTO/JETSET Ÿ ˆ ƒ Ÿ.. ² ± Ì,. Œ. ŠÊ Íμ,.. μ ± Ö 1, Œ. ƒ. μ ±μ Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê Ò Ê²ÓÉ ÉÒ ³ ÒÌμ μ ÉÖ ²ÒÌ μ μ É μ μ ²Ê μ±μ - Ê Ê μ³ Ö

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering

P ˆ.. ƒê ²μ 1,.. Œ ² ±μ 1,..Šμ Í,.. ʳ,.. μ μ 2. ˆ ˆŸ Š Š ˆ ƒ ˆŒ œ ƒ Œ ƒ ƒ Š-Š ˆ 10- Œ ˆ. ( ), Œμ ± Œμ ± 1 μ Ò É Ì μ²μ ±μ³ μ ÉÒ ±Êʳ ÒÌ μ μ

P9-2017-78 ˆ.. ƒê ²μ 1,.. Œ ² ±μ 1,..Šμ Í,.. ʳ,.. μ μ 2 ˆ ˆŸ Š Š ˆ ƒ ˆŒ œ ƒ Œ ƒ ƒ Š-Š ˆ 10- Œ ˆ 1 μ Ò É Ì μ²μ ±μ³ μ ÉÒ ±Êʳ ÒÌ μ μ ( ), Œμ ± 2 Œμ ±μ ± μ Ê É Ò Ê É É ³. Œ.. μ³μ μ μ, Œμ ± ƒê ²μ ˆ... P9-2017-78

Studies on the Binding Mechanism of Several Antibiotics and Human Serum Albumin

2005 63 Vol. 63, 2005 23, 2169 2173 ACTA CHIMICA SINICA No. 23, 2169 2173 a,b a a a *,a ( a 130012) ( b 133002), 26 K A 1.98 10 4, 1.01 10 3, 1.38 10 3, 5.97 10 4 7.15 10 4 L mol 1, n 1.16, 0.86, 1.19,

Ó³ Ÿ , º 7(163).. 793Ä797 ˆ ˆŠ ˆ ˆŠ Š ˆ. .. Ëμ μ. Î ± É ÉÊÉ ³..., Œμ ±

Ó³ Ÿ. 2010.. 7, º 7(163).. 793Ä797 ˆ ˆŠ ˆ ˆŠ Š ˆ Š ˆ œ Š Œ ˆ Œ.. Ëμ μ Î ± É ÉÊÉ ³..., Œμ ± ² É Î ± ³μÉ μ Ëμ ³ μ ²Ó μéμî ÒÌ Ô² ±É μ ÒÌ Êαμ, Ö ±μéμ ÒÌ Î É Î μ É ² μ μ ³, Éμ± ³, ÒÏ ÕÐ ³ ²Ó μ Î Éμ± ²Ó. Ê

EPS-HEP 2015 DOUBLE-SCATTERING MECHANISM. Antoni Szczurek 1,2 Mariola Kłusek-Gawenda 1

EPS-HEP 5 DOUBLE-SCTTERING MECHNISM OF PRODUCTION OF TWO MESONS IN ULTRPERIPHERL, ULTRRELTIISTIC HEY ION COLLISIONS ntoni Szczurek, Mariola Kłusek-Gawenda Institute of Nuclear Physics PN Kraków University

Non-Gaussianity from Lifshitz Scalar

COSMO/CosPA 200 September 27, 200 Non-Gaussianity from Lifshitz Scalar Takeshi Kobayashi (Tokyo U.) based on: arxiv:008.406 with Keisuke Izumi, Shinji Mukohyama Lifshitz scalars with z=3 obtain super-horizon,

[1] P Q. Fig. 3.1

1 (a) Define resistance....... [1] (b) The smallest conductor within a computer processing chip can be represented as a rectangular block that is one atom high, four atoms wide and twenty atoms long. One

Š ˆ œ Ÿ ˆ œ Œ Œ ƒ ˆ Œ Œ LEPTA

Ó³ Ÿ. 2006.. 3, º 7(136).. 78Ä83 Š 537.533.33, 621.384.60-833 Š ˆ œ Ÿ ˆ œ Œ Œ ƒ ˆ Œ Œ LEPTA ( ).. μ²éêï±,.. Ò±μ ±,. ƒ. Šμ Í,.. Šμ μé,. ˆ. μì³ Éμ,.. Œ ² Ìμ, ˆ.. Œ ϱμ,.. ²μ,.., ˆ.. ²,.. μ,.. ³ μ,. Œ. Ò,

Engineering Tunable Single and Dual Optical. Emission from Ru(II)-Polypyridyl Complexes. Through Excited State Design

Engineering Tunable Single and Dual Optical Emission from Ru(II)-Polypyridyl Complexes Through Excited State Design Supplementary Information Julia Romanova 1, Yousif Sadik 1, M. R. Ranga Prabhath 1,,

2.1

181 8588 2 21 1 e-mail: sekig@th.nao.ac.jp 1. G ab kt ab, (1) k 8pGc 4, G c 2. 1 2.1 308 2009 5 3 1 2) ( ab ) (g ab ) (K ab ) 1 2.2 3 1 (g ab, K ab ) 1 t a S n a a b a 2.3 a b i (t a ) 2 1 2.4 1 g ab ab

Φυσική Στοιχειωδών Σωματιδίων ΙΙ (8ου εξαμήνου) Χ. Πετρίδου, Κ. Κορδάς. Μάθημα 2β: Πειράματα-Ανιχνευτές

Φυσική Στοιχειωδών Σωματιδίων ΙΙ (8ου εξαμήνου) Χ. Πετρίδου, Κ. Κορδάς Μάθημα 2β: Πειράματα-Ανιχνευτές Λέκτορας Κώστας Κορδάς Αριστοτέλειο Πανεπιστήμιο Θεσσαλονίκης Στοιχειώδη ΙΙ, Αριστοτέλειο Παν. Θ/νίκης,

2. Laser Specifications 2 1 Specifications IK4301R D IK4401R D IK4601R E IK4101R F. Linear Linear Linear Linear

2. Laser Specifications 2 1 Specifications IK4301R D IK4401R D IK4601R E IK4101R F 441.6 441.6 441.6 441.6 30 50 70 100 TEM00 TEM00 TEM00 TEM00 BEAM DIAMETER ( 1/e2) 1.1 1.1 1.2 1.2 0.5 0.5 0.5 0.4 RATIO

γ c = rl = lt R ~ e (g l)t/t R Intensität 0 e γ c t Zeit, ns

There is however one main difference in this chapter compared to many other chapters. All loss and gain coefficients are given for the intensity and not the amplitude and are therefore a factor of 2 larger!

100102; 2. Fe Cu Hg. Rapid multi-elemental analysis on four precious Tibetan medicines based on LIBS technique

2015 6 40 11 Vol. 40 No. 11 June 2015 LIBS 4 1,2, 1,2, 1,2, 1,2, 1,2* 1,2*, ( 1., 100102; 2., 100102) LIBS 4 4 Nd YAG 1 064 nm NIST LIBS 4 Ca Na K Mg C-N Fe Cu Hg Ag LIBS 4 LIBS Rapid multi-elemental analysis

Aτοµική Δοµή LASER. Τροχιές ηλεκτρονίων Ατοµικά Φάσµατα Άτοµο Bohr

Τροχιές ηλεκτρονίων Ατοµικά Φάσµατα Άτοµο Bohr Aτοµική Δοµή LASER Ενεργειακά Επίπεδα και Φάσµατα Αρχή της Αντιστοιχίας Πυρηνική Κίνηση Ατοµική Διέγερση Laser Light Amplification by Stimulated Emission

Fused Bis-Benzothiadiazoles as Electron Acceptors

Fused Bis-Benzothiadiazoles as Electron Acceptors Debin Xia, a,b Xiao-Ye Wang, b Xin Guo, c Martin Baumgarten,*,b Mengmeng Li, b and Klaus Müllen*,b a MIIT Key Laboratory of ritical Materials Technology

Quantum shot noise: From Schottky to Bell

Quantum shot noise: From Schottky to Bell Markus Büttiker University of Geneva Peter Samuelsson Eugene V. Sukhorukov Vanessa Chung Valentin Rytchkov Micheal Polianski Micheal Moskalets Niels Bohr Summer

CONSULTING Engineering Calculation Sheet

E N G I N E E R S Consulting Engineers jxxx 1 Structure Design - EQ Load Definition and EQ Effects v20 EQ Response Spectra in Direction X, Y, Z X-Dir Y-Dir Z-Dir Fundamental period of building, T 1 5.00

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts

Written Examination. Antennas and Propagation (AA ) April 26, 2017.

Written Examination Antennas and Propagation (AA. 6-7) April 6, 7. Problem ( points) Let us consider a wire antenna as in Fig. characterized by a z-oriented linear filamentary current I(z) = I cos(kz)ẑ

1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 β Transitions

1 Decay Scheme Le césium se désintègre essentiellement par émission bêta moins vers des niveaux excités du baryum. Cs- desintegrates mainly by beta minus emissions to excited levels in Ba-. 2 Nuclear Data

Answers to practice exercises

Answers to practice exercises Chapter Exercise (Page 5). 9 kg 2. 479 mm. 66 4. 565 5. 225 6. 26 7. 07,70 8. 4 9. 487 0. 70872. $5, Exercise 2 (Page 6). (a) 468 (b) 868 2. (a) 827 (b) 458. (a) 86 kg (b)

Tunable Diode Lasers. Turning Laser Diodes into Diode Lasers. Mode selection. Laser diodes

Tunable Diode Lasers Turning Laser Diodes into Diode Lasers Laser diodes Mode selection FP diodes high power at low cost AR diodes for best performance Compact and robust Littrow setup Highest power from

An experimental and theoretical study of the gas phase kinetics of atomic chlorine reactions with CH 3 NH 2, (CH 3 ) 2 NH, and (CH 3 ) 3 N

Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2015 An experimental and theoretical study of the gas phase kinetics of atomic chlorine

Fundamental Physical Constants Complete Listing Relative std. Quantity Symbol Value Unit uncert. u r

UNIVERSAL speed of light in vacuum c, c 0 299 792 458 m s 1 (exact) magnetic constant µ 0 4π 10 7 NA 2 = 12.566 370614... 10 7 NA 2 (exact) electric constant 1/µ 0 c 2 ε 0 8.854 187 817... 10 12 Fm 1 (exact)

1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions

1 Decay Scheme Bi- disintegrates 97.91(3) % by beta minus emission to the levels in Po- and 2.09(3) % through alpha decay to Tl-209. Le bismuth se désintègre principalement par émissions bêta vers le polonium

Supporting Information

Supporting Information Aluminum Complexes of N 2 O 2 3 Formazanate Ligands Supported by Phosphine Oxide Donors Ryan R. Maar, Amir Rabiee Kenaree, Ruizhong Zhang, Yichen Tao, Benjamin D. Katzman, Viktor

ˆ ˆ ˆ ˆˆ γ-ˆ ˆŸ ˆ Š Œ ˆ Œ œ Š ˆˆ

Ó³ Ÿ. 2008.. 5, º 2(144).. 219Ä225 ˆ ˆ ƒˆÿ, Š ƒˆÿ ˆ Ÿ Ÿ Œ ˆ ˆ ˆ ˆ ˆ Œ Œ ˆ ˆ ˆ ˆˆ γ-ˆ ˆŸ ˆ Š Œ ˆ Œ œ Š ˆˆ.. Šμ ²μ a,.. Š,.. μ ±μ,.. Ö a,.. ² ± a,.. ² Õ± a a ÊÎ μ- ² μ É ²Ó ± É ÉÊÉ Ö μ Ë ± ³... ±μ ²ÓÍÒ Œμ

MATSEC Intermediate Past Papers Index L. Bonello, A. Vella

2009 MATSEC Intermediate Past Papers Index Louisella Bonello Antonia Vella The Junior College Physics Department 2009 MATSEC INTERMEDIATE PAST PAPERS INDEX WITH ANSWERS TO NUMERICAL PROBLEMS by Louisella

Δ. Σαμψωνίδης & Κ.Κορδάς. Ανιχνευτές : Μάθημα 1β Αλληλεπίδραση ακτινοβολίας με την ύλη.

Επταχθντές - Ανιχνευτές Δ. Σαμψωνίδης & Κ.Κορδάς Ανιχνευτές : Μάθημα 1β Αλληλεπίδραση ακτινοβολίας με την ύλη. Κώστας Κορδάς Αριστοτέλειο Πανεπιστήμιο Θεσσαλονίκης Επιταχυντές & Ανιχνευτές 8ου εξαμήνου,

P Ò±,. Ï ± ˆ ˆŒˆ Š ƒ ˆŸ. Œ ƒ Œ ˆˆ γ-š Œˆ ƒ ƒˆ 23 ŒÔ. ² μ Ê ². Í μ ²Ó Ò Í É Ö ÒÌ ² μ, É μí±, μ²óï

P15-2012-75.. Ò±,. Ï ± ˆ Œ ˆŸ ˆ, š Œ ˆ ˆŒˆ Š ƒ ˆŸ ˆ ˆ, Œ ƒ Œ ˆˆ γ-š Œˆ ƒ ƒˆ 23 ŒÔ ² μ Ê ² Í μ ²Ó Ò Í É Ö ÒÌ ² μ, É μí±, μ²óï Ò±.., Ï ±. P15-2012-75 ˆ ³ Ö μ Ì μ É, μ Ñ ³ ÒÌ μ É Ì ³ Î ±μ μ μ É μ Íμ Ö ÕÐ

Αναζητώντας παράξενα σωµατίδια στο ALICE

Αναζητώντας παράξενα σωµατίδια στο ALICE K 0 s π+ π - Λ π - p Ξ - π - Λ π - p π - 7.7.018 Δέσποινα Χατζηφωτιάδου 1 παράξενα σωµατίδια µεσόνιο βαριόνιο s K 0 s ds, ds Λ uds αδρόνια που περιέχουν τουλάχιστον

Επιταχυντές Χαμηλών Ενεργειών

Επιταχυντές Χαμηλών Ενεργειών Α. Λαγογιάννης Ινστιτούτο Πυρηνικής και Σωματιδιακής Φυσικής Είδη Επιταχυντών Επιταχυντής: Διάταξη που μεταδίδει ενέργεια σε φορτισμένα σωμάτια και ιόντα και τα συγκρατεί

Constitutive Relations in Chiral Media

Constitutive Relations in Chiral Media Covariance and Chirality Coefficients in Biisotropic Materials Roger Scott Montana State University, Department of Physics March 2 nd, 2010 Optical Activity Polarization

1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions

1 Decay Scheme I- disintegrates by electron capture mainly via the 159 level of Te- (97%). L iode se désintègre par capture électronique principalement vers le niveau excité de 159 du tellure, avec une

Τοίχοι Ωπλισμένης Γής: υναμική Ανάλυση Πειράματος Φυγοκεντριστή. Reinforced Soil Retaining Walls: Numerical Analysis of a Centrifuge Test

Τοίχοι Ωπλισμένης Γής: υναμική Ανάλυση Πειράματος Φυγοκεντριστή Reinforced Soil Retaining Walls: Numerical Analysis of a Centrifuge Test ΓΕΡΟΛΥΜΟΣ, Ν. Πολιτικός Μηχανικός, Λέκτορας, Ε.Μ.Π. ΖΙΩΤΟΠΟΥΛΟΥ,

ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ Ä616 Š ˆŒ CMS LHC

ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ 2017.. 48.. 5.. 604Ä616 œ ˆ Š ˆ ˆ ˆ Š ˆŒ CMS LHC ˆ.. ƒμ²êé 1,.. ³ Éμ 1,2, 1 Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê 2 ƒμ Ê É Ò Ê É É Ê, Ê, μ Ö É ² Ò Ê²ÓÉ ÉÒ Ô± ³ É CMS, μ²êî Ò μ μ ÒÌ - μ μ Í ±² μéò LHC

Properties of a Some (Ag-Cu-Sn) Alloys for Shielding Against Gamma Rays

, pp.35-46 http://dx.doi.org/10.14257/ijast.2014.63.04 Properties of a Some (Ag-Cu-Sn) Alloys for Shielding Against Gamma Rays M. A. M. Uosif Physics Department, Faculty of Science, Al-Azher University,

Th, Ra, Rn, Po, Pb, Bi, & Tl K x-rays. Rn Kα1. Rn Kα2. 93( 227 Th)/Rn Kβ3. Ra Kα2. Po Kα2 /Bi K α1 79( 227 Th)/Po Kα1. Ra Kα1 /Bi K β1.

Page -1-10 8 10 7 10 6 10 5 10 4 334 ( Th) Counts/Channel 10 3 10 2 10 1 49 ( Th)/ 50 ( Th)/ 50 ( Fr) 0 100 200 300 400 500 600 700 800 900 1000 1000 1100 1200 1300 1400 1500 1600 1700 1800 1900 2000 Channel

Problem 7.19 Ignoring reflection at the air soil boundary, if the amplitude of a 3-GHz incident wave is 10 V/m at the surface of a wet soil medium, at what depth will it be down to 1 mv/m? Wet soil is

Contents X-ray Fluorescence (XRF) and Particle-Induced X-ray Emission (PIXE)

Contents 1 X-ray Fluorescence (XRF) and Particle-Induced X-ray Emission (PIXE)... 1 1.1 Introduction............................................ 1 1.2 PrincipleofXRFandPIXETechniques... 2 1.3 Theory and

difluoroboranyls derived from amides carrying donor group Supporting Information

The influence of the π-conjugated spacer on photophysical properties of difluoroboranyls derived from amides carrying donor group Supporting Information Anna Maria Grabarz a Adèle D. Laurent b, Beata Jędrzejewska

P ƒ. μ μ², Œ.. ˆ μ,.. μ ± Î Š Ÿ ˆ Œ ˆŸ ˆ Ÿ Š ˆ. ² μ Ê ² μ Ò É Ì ± Ô± ³ É.

P13-2011-120. ƒ. μ μ², Œ.. ˆ μ,.. μ ± Î Š Ÿ ˆ Œ ˆŸ ˆ Ÿ Š ˆ ² μ Ê ² μ Ò É Ì ± Ô± ³ É E-mail: sobolev@nrmail.jinr.ru μ μ². ƒ., ˆ μ Œ.., μ ± Î.. P13-2011-120 É μ ± ²Ö ³ Ö μ² ÒÌ Î Ö ÒÌ ±Í Ò É Ö Ô± ³ É ²Ó Ö

Study of In-vehicle Sound Field Creation by Simultaneous Equation Method

Study of In-vehicle Sound Field Creation by Simultaneous Equation Method Kensaku FUJII Isao WAKABAYASI Tadashi UJINO Shigeki KATO Abstract FUJITSU TEN Limited has developed "TOYOTA remium Sound System"

Dirac Trace Techniques

Dirac Trace Techniques Consider a QED amplitude involving one incoming electron with momentum p and spin s, one outgoing electron with momentum p and spin s, and some photons. There may be several Feynman

Metal Oxide Varistors (MOV) Data Sheet

Φ SERIES Metal Oxide Varistors (MOV) Data Sheet Features Wide operating voltage (V ma ) range from 8V to 0V Fast responding to transient over-voltage Large absorbing transient energy capability Low clamping

1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions

1 Decay Scheme U- disintegrates by alpha emission mainly to the ground and 49- states in Th-232, and by 9,3 10 8 % spontaneous fission. L uranium se désintègre par émission alpha et par fission spontanée

What happens when two or more waves overlap in a certain region of space at the same time?

Wave Superposition What happens when two or more waves overlap in a certain region of space at the same time? To find the resulting wave according to the principle of superposition we should sum the fields

Ó³ Ÿ , º 3(201).. 461Ä ƒ. ÒÏ ±,.. μ 1. ˆ É ÉÊÉ Ö ÒÌ μ ² ³ ²μ Ê ±μ μ μ Ê É μ μ Ê É É, Œ ±

Ó³ Ÿ. 2016.. 13, º 3(201).. 461Ä470 ˆ ˆŠ Œ ˆ ˆ Œ ƒ Ÿ. ˆŸ Œ ˆ ( ˆ ˆ ˆ ˆ ˆ Œ) Š ƒˆˆ. ƒ. ÒÏ ±,.. μ 1 ˆ É ÉÊÉ Ö ÒÌ μ ² ³ ²μ Ê ±μ μ μ Ê É μ μ Ê É É, Œ ± Ÿ ² μ μ μ ²ÊÎ ²μ³² Ö ( μ μ μé μ Ò Ì μ ³) É μ μ μ²ó- Ïμ

Š ƒ ˆŠ œ ˆ ˆ ˆ Œ ƒ ˆ Š ˆˆ Š

Ó³ Ÿ. 204.., º 4(88).. 768Ä776 ˆ ˆŠ ˆ ˆŠ Š ˆ Š ƒ ˆŠ œ ˆ ˆ ˆ Œ ƒ ˆ Š ˆˆ Š Š ˆ Œ ˆ Š Œ ˆ Œ. Œ. Ò Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê ËË ±É μ ÉÓ ³ μ μμ μ μé μ ±Í μ μ μ²ó μ ³ Ô² ±É μ μ μ μì² Ö É μé ÊÌ ³ É μ : ÔËË ±É μ É

ΑΡΧΕΣ ΤΗΛΕΠΙΣΚΟΠΗΣΗΣ (Y2204) Βασιλάκης Εµµανουήλ Λέκτορας Τηλεανίχνευσης

ΑΡΧΕΣ ΤΗΛΕΠΙΣΚΟΠΗΣΗΣ (Y2204) Βασιλάκης Εµµανουήλ Λέκτορας Τηλεανίχνευσης ΘΕΜΑΤΑ Τι είναι τηλεπισκόπηση Ιστορική εξέλιξη Συστήµατα παρατήρησης της Γης Στοιχεία Ηλεκτρο-Μαγνητικής Ακτινοβολίας Διακριτική

First Sensor Quad APD Data Sheet Part Description QA TO Order #

Responsivity (/W) First Sensor Quad PD Data Sheet Features Description pplication Pulsed 16 nm laser detection RoHS 211/65/EU Light source positioning Laser alignment ø mm total active area Segmented in

Dipole-Guided Electron Capture Causes Abnormal Dissociations of Phosphorylated Pentapeptides

Supplementary Material for Dipole-Guided Electron Capture Causes Abnormal Dissociations of Phosphorylated Pentapeptides Christopher L. Moss, a Thomas W. Chung, a Jean A. Wyer, b Steen Brøndsted Nielsen,

Φυσική Στοιχειωδών Σωµατιδίων ΙΙ. Μάθηµα 1ο 15/2/2011

Φυσική Στοιχειωδών Σωµατιδίων ΙΙ Μάθηµα 1ο 15/2/2011 Τι θα συζητήσουμε σήμερα Γενικά στοιχεία για τα πειράματα Στοιχειωδών σωματιδίων Γενικά - χαρακτηριστικά επιταχυντών ηλεκτρικά και μαγνητικά πεδία Γραμμικοί

Quantum dot sensitized solar cells with efficiency over 12% based on tetraethyl orthosilicate additive in polysulfide electrolyte

Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 2017 Supplementary Information (SI) Quantum dot sensitized solar cells with