'Sin 2' diaporamas de présentation

Sin 2 - PowerPoint PPT Presentation


Outline

Outline

“ 4 th generation” and B-CP anomalies PHENO09 Amarjit Soni HET, BNL adlersoni@gmail.com,soni@bnl.gov. Outline. Motivation FOUR ANOMALIES A NATURAL solution that fits the pattern of anomalies Broader repercussions Conclusion & Summary. Motivation.

By Renfred
(272 views)

A New Experiment To Measure θ 13

A New Experiment To Measure θ 13

A New Experiment To Measure θ 13. David Reyna Argonne National Laboratory. CKM Matrix. MNS Matrix. 3 Flavor Mixing Matrix. Mixing Angles. Matrix Components: 3 Euler Angles ( θ 12 ; θ 13 ; θ 23 ) 1 CP phase ( δ ) (+2 Majorana Phases). Atmospheric ( ν μ ν x ). Solar ( ν e ν x ).

By Gideon
(616 views)

Credit revision Q 1

Credit revision Q 1

Credit revision Q 1. What is the sine rule ?. Credit revision Q 2. What three processes do you go through in order to factorise a quadratic ?. Credit revision Q 3. What is sin x cos x equal to ?. Credit revision Q 4. How do you solve equations of the form

By betty_james
(211 views)

EMT 101 – Engineering Programming

EMT 101 – Engineering Programming

Week 11. EMT 101 – Engineering Programming. Dr. Farzad Ismail. School of Aerospace Engineering Universiti Sains Malaysia Nibong Tebal 14300 Pulau Pinang. Extensive Library Package. One of the best features in MATLAB is that it has a more extensive library package compared to C++

By andrew
(369 views)

New Hadron Spectroscopies

New Hadron Spectroscopies

New Hadron Spectroscopies. Stephen L. Olsen University of Hawai’i. d. u. u. d. s. d. c. d. c. c. c. History:. chadwick. 1930’s: proton & neutron ..all we need??? 1950’s: ,,,,,… “Had I foreseen that, I would have gone into botany” – Fermi

By payton
(148 views)

DIS-Parity 12 GeV

DIS-Parity 12 GeV

DIS-Parity 12 GeV. Kent Paschke University of Massachusetts. Physics opportunities in PVeS with a Solenoidal Spectrometer. Many slides liberated from: P. Souder, K. Kumar (… and their sources). PV Asymmetries. Weak Neutral Current (WNC) Interactions at Q 2 << M Z 2.

By kiana
(340 views)

Reynolds-Averaged Navier -Stokes Equations -- RANS

Reynolds-Averaged Navier -Stokes Equations -- RANS

Reynolds-Averaged Navier -Stokes Equations -- RANS. 4 equations; 7 unknowns. Similar situation as when we went from Cauchy’s eq to N-S eq. A j = eddy viscosity. [m 2 /s]. Turbulence Closure. Turbulent Kinetic Energy (TKE). Total flow = Mean plus turbulent parts =. Same for a scalar:.

By nixie
(407 views)

CHE-20031 ( S tructural I norganic C hemistry) X-ray Diffraction & Crystallography lecture 2

CHE-20031 ( S tructural I norganic C hemistry) X-ray Diffraction & Crystallography lecture 2

CHE-20031 ( S tructural I norganic C hemistry) X-ray Diffraction & Crystallography lecture 2. Dr Rob Jackson LJ1.16, 01782 733042 r.a.jackson@keele.ac.uk www.facebook.com/robjteaching Twitter: #che20031. X-ray Diffraction & Crystallography: lecture 2 plan.

By mahsa
(298 views)

Sine and Cosine graphs

Sine and Cosine graphs

Section 4.5. Sine and Cosine graphs. SIN graphs. 1.) y = sin Θ. 2.) y = 2 sin Θ. SIN graphs. 3.) y = ½ sin Θ. 4.) y = sin 2 Θ. SIN graphs. 5.) y = sin 3 Θ. 6.) y = sin ½ Θ. SIN graphs. 7.) y = -sin Θ. 8.) y = -2 sin 3 Θ. Sin graphs. COS graphs. 1.) y = cos Θ.

By brianna
(115 views)

The Debye-Waller factor Start w/ structure factor 	F hkl =  f n exp (2 π i r *  r n )

The Debye-Waller factor Start w/ structure factor F hkl =  f n exp (2 π i r *  r n )

The Debye-Waller factor Start w/ structure factor F hkl =  f n exp (2 π i r *  r n ). hkl. unit cell. S / . (S -S o )/ . 2 . S o / . | r *| = | s - s o |/  = (2 sin  )/ . r * = ( s - s o )/  = h a * + k b * + l c * r = x a + y b + z c. For small  r n

By jesse
(144 views)

Matlab - Fourier Analysis

Matlab - Fourier Analysis

Matlab - Fourier Analysis. 主講人:林麗娟 主講部分: FFT & 例題. Fourier Transform. 連續時間 下的 Fourier Transform 定義:. 離散時間 下的 Fourier Transform 定義﹝ DTFT﹞:. Fourier Transform. 無限 的 Discrete Fourier transform 定義﹝ DTFT﹞:. 有限 的 Discrete Fourier Transform 定義﹝ DFT﹞:. Compare DTFT & DFT.

By yoland
(185 views)

§12 . 9 二阶常系数非齐次线性微分方程

§12 . 9 二阶常系数非齐次线性微分方程

§12 . 9 二阶常系数非齐次线性微分方程. 二阶常系数非齐次线性微分方程. 一、 f ( x ) = P m ( x ) e l x 型. 特解形式. 二、 f ( x ) = e l x [ P l ( x )cos w x + P n ( x )sin w x ] 型. 特解形式. 二阶常系数非齐次线性微分方程. 二阶常系数非齐次线性微分方程:. 是形如 y  + py  + qy = f ( x ) 的方程,其中 p 、 q 是常数.. 二阶常系数非齐次线性微分方程通解的结构:. 设齐次方程

By linus
(128 views)

Neutrino Oscillation Experiment between JHF – Super-Kamiokande

Neutrino Oscillation Experiment between JHF – Super-Kamiokande

Neutrino Oscillation Experiment between JHF – Super-Kamiokande. Yoshihisa OBAYASHI (Kamioka Observatory, ICRR). JHF Neutrino Working Group. Y. Itow, Y. Obayashi , Y. Totsuka (ICRR) Y. Hayato, H. Ishino, T. Kobayashi, K. Nakamura, M. Sakuda (KEK) T. Hara (Kobe)

By neviah
(132 views)

Accelerator and Detector

Accelerator and Detector

Accelerator and Detector. KEK-B accelerator. Two separate rings: 8GeV(e - )/3.5GeV(e + ). Finite crossing angle. Design luminosity = 10 34 cm -2 sec -1. Achieved lum =1.06  10 34 cm -2 sec -1. Belle logged: 158 fb -1. KEKB Collider.

By maja
(76 views)

Warm Up

Warm Up

Sin (A – B) = Tan (2B) = Tan =. Warm Up. Simplifying Trig Expressions using Fundamental Identities. Reciprocal Identities. Quotient Identities. Examples: Simplify Completely. Examples: Simplify Completely. ( cos x )( csc x ) =. A. 1 B. tan 2 x C. -1 D. cot 2 x.

By gizela
(73 views)

FIT 1005 Networks & Data Communications

FIT 1005 Networks & Data Communications

FIT 1005 Networks & Data Communications. Lecture 2 – Data Transmission Reference: Chapter 3 Data and Computer Communications Eighth Edition by William Stallings Lecture slides by Lawrie Brown Lecture slides also available at : http://users.monash.edu.au/~amkhan/fit1005/.

By latika
(175 views)

Ilana HARRUS (USRA/NASA/GSFC)

Ilana HARRUS (USRA/NASA/GSFC)

Continuum Processes (in High-Energy Astrophysics) 3rd X-ray Astronomy school Wallops Island May 12-16 May. Ilana HARRUS (USRA/NASA/GSFC). Bremsstrahlung. What is Bremsstrahlung? (and why this bizarre name of “braking radiation”?)

By markku
(89 views)

Daya Bay Reactor Neutrino Experiment

Daya Bay Reactor Neutrino Experiment

Daya Bay Reactor Neutrino Experiment. Even More. Bob McKeown (for the Daya Bay collaboration) California Institute of Technology. Precise Measurement of q 13. DOANOW, Honolulu, Hawaii, March 24, 2007. Outline. Physics Motivation Requirements The Daya Bay experiment Layout

By maia
(161 views)

Ch 2 - Fundamentals of Seismic Exploration I. Seismic waves and wave propagation

Ch 2 - Fundamentals of Seismic Exploration I. Seismic waves and wave propagation

Ch 2 - Fundamentals of Seismic Exploration I. Seismic waves and wave propagation view waves as emanating spherically from a point source pebble in water earthquake we need to know about: wave type (surface vs body) factors controlling transmission of energy wave speed

By tiger
(161 views)

ABSOLUTE MOTION ANALYSIS (Section 16.4)

ABSOLUTE MOTION ANALYSIS (Section 16.4)

ABSOLUTE MOTION ANALYSIS (Section 16.4). Today’s Objective : Students will be able to determine the velocity and acceleration of a rigid body undergoing general plane motion using an absolute motion analysis. In-Class Activities : • Check homework, if any • Reading quiz • Applications

By arty
(426 views)

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