“Amplitude Cooling” in Step III & IV Timothy Carlisle.

Slides:



Advertisements
Similar presentations
CM31: Multiple Scattering in GEANT4 Timothy Carlisle University of Oxford.
Advertisements

Emittance definition and MICE staging U. Bravar Univ. of Oxford 1 Apr Topics: a) Figure of merit for MICE b) Performance of MICE stages.
Tracker Reconstruction Stuff Timothy Carlisle Oxford.
MICE analysis meeting - (01/06/2006) 1 few words on emittance growth in step III M. Apollonio – University of Oxford.
1 EMCal & PID Rikard Sandström Universite de Geneve MICE collaboration meeting 26/6-05.
1 PID, emittance and cooling measurement Rikard Sandström University of Geneva MICE Analysis phone conference.
MICE analysis meeting - (4/5/2006) 1 some reflections on scraping, PID sizes and Transmittance M. Apollonio – University of Oxford.
Alain Blondel MICE: Constraints on the solenoids 2.Field Homogeneity: or ? this will be dictated by the detector requirements. TPG will be.
OPTICS UPDATE Ulisse Bravar University of Oxford 3 August 2004.
1 Downstream scraping and detector sizes Rikard Sandström University of Geneva MICE collaboration meeting CERN.
Downstream transversal sizes Rikard Sandström University of Geneva MICE detector meeting.
1 Muon Yield Comparisons for Different ICOOL Versions and Lattices X. Ding Front End, Nov. 23, 2010.
MICE analysis meeting - (6/4/2006) 1 Update on MICE – step III M. Apollonio – University of Oxford.
MICE analysis meeting - (21/09/2006) 1 Transmittance, scraping and maximum radii for MICE STEPVI M. Apollonio – University of Oxford.
1 G4MICE downstream distributions G4MICE plans Rikard Sandström Universite de Geneve MICE collaboration meeting 27/6-05.
Tracker Misalignment Study David Forrest CM23 HIT, Harbin January 14 th.
MICE analysis meeting - (26/3/2006) 1 Update on MICE – step III M. Apollonio – University of Oxford.
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
M.apollonioAM STEPIII – sizes and positioning m.apollonio, Oxford.
MICE CM - Fermilab, Chicago - (11/06/2006) 1 A (short) history of MICE – step III M. Apollonio – University of Oxford.
Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin.
1. Optical matching in MICE Ulisse Bravar University of Oxford 2 June 2004 Constraints Software MICE proposal mismatch MICE Note 49 (September 2004, Bob.
24 Nov 2009PC Analysis PC Schedule 2009 Tuesdays fortnightly Proposed dates: 13 October  27 October  CM25 4 – 6 November  24 November 8 December.
M.apollonioImperial College - London1 M. Apollonio University of Oxford the MICE diffuser: issues and operation MICE beamline review Nov. 16 th 2007 Imperial.
Beam Parameter Study - preliminary findings Tim Carlisle.
MICE Project Board Alain Blondel 1 MICE running Preamble ISIS running Step I Step(s) IV Step V (and VI)
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=

M.apollonioam M. Apollonio University of Oxford update on STEP III.
Diffuser Studies Chris Rogers, IC/RAL MICE VC 09 March 2005.
Timothy Carlisle, Oxford CM 28. Step 3 Matching Step 3  Step 3 rematched for 830 mm spool piece  Calc. B(z) & BetaFn with the following:  Minimize.
Emittance measurement: ID muons with time-of-flight Measure x,y and t at TOF0, TOF1 Use momentum-dependent transfer matrices iteratively to determine trace.
Emittance measurement: ID muons with time-of-flight Measure x,y and t at TOF0, TOF1 Use momentum-dependent transfer matrices to map  path Assume straight.
TJR 01/21/2003Slide 1 Simulations of the Study 2 Cooling Channel with Realistic Absorber Windows Tom Roberts Illinois Institute of Technology.
Multiple Scattering (MSC) in Geant4 Timothy Carlisle Oxford.
Marco apollonio/J.CobbMICE coll. meeting 16- RAL - (10/10/2006) 1 Transmittance, scraping and maximum radii for MICE STEPVI M. Apollonio – University of.
Step IV Studies Timothy Carlisle Oxford. Intro. CM28 – Step III vs Step IV Cooling formula & G4MICE disagree on – Also observed in ICOOL (note #199 –
Inv The Pendulum Question: What is the relationships between the frequency of a simple pendulum and its mass, amplitude and length? Materials: refer.
Yoyo points 38 points M2 Amp. 383.
Re-tuning MICE June 1 st 2010 Tim Carlisle. Intro At the moment MICE coil currents optimized for: central Pz = 0 RF No LH2 want to rematch M1 & M2 in.
Measuring Multiple Scattering in Step IV Timothy Carlisle Oxford See MICE Note 374 for updated results.
1 OPTICS OF MICE STEP V.0 Ulisse Bravar University of New Hampshire 26 June 2005.
实验十四 紫外线灭菌  一、实验背景及目的:  灭菌是一种杀灭微生物的措施。紫外线灭菌 是物理灭菌因素之一。  1. 了解紫外线灭菌的原理;  2. 学习、掌握紫外线灭菌的方法。 版权所有 未经作者同意 请勿使用.
Лучевая диагностика заболеваний пищевого канала
Mark Rayner – Analysis SessionCM25, 4 November The TOF detectors: Beyond particle identification Mark Rayner The University of Oxford MICE CM25.
(one of the) Request from MPB
MICE S TEP IV P HYSICS ‘D ELIVERABLES ’ V. Blackmore MAP 2014 Spring Meeting 30 th May, /15 AKA “What will we learn from Step IV?”
CM Nov 2009 DOES MICE NEED STEP III ? Somewhat hard to understand MICE Schedule… –If the gods are (un)kind it’s possible that SS1, SS2 & FC1 are.
The reading is 7.38 mm. The reading is 7.72 mm.
Презентацию подготовила Хайруллина Ч.А. Муслюмовская гимназия Подготовка к части С ЕГЭ.
ΟΡΓΑΝΩΣΗ ΚΑΙ ΔΙΟΙΚΗΣΗ ΕΠΙΧΕΙΡΗΣΕΩΝ 3 Ο ΜΑΘΗΜΑ. ΟΙ ΜΕΓΑΛΕΣ ΕΠΙΧΕΙΡΗΣΕΙΣ Η δημιουργία μεγάλων επιχειρήσεων είναι ένα από τα χαρακτηριστικά του 20 ου αιώνα.
10 mm is the same as... 1 cm. 20 mm is the same as... 2 cm.
输尿管软镜钬激光碎石术的体会 南华大学附属第二医院泌尿外科三区 钱 坤. 背 景  输尿管软镜作为一种新碎石手段,目前在部分医 院应用。其安全性、有效性得到一致的认可。  但是存在一些问题需要探讨:  手术适应症、禁忌症  影响碎石成功率的因素  手术并发症的防治.
Beam Energy-Loss measurement
Field-on measurement of multiple scattering
Tips Need to Consider When Organizing a College Event
ФОНД ЗА РАЗВОЈ РЕПУБЛИКЕ СРБИЈЕ
ОПШТИНА КУРШУМЛИЈА.
ماجستير إدارة المعارض من بريطانيا
ОПЕРАТИВНА ПРОГРАМА “ИНОВАЦИИ И КОНКУРЕНТОСПОСОБНОСТ“ „Подобряване на производствения капацитет в МСП“
'III \-\- I ', I ,, - -
Area of a rectangle Tuesday, 05 February 2019 Definition:
Index Notation Sunday, 24 February 2019.
ХУД 34-р сургуулийн нийгмийн ухааны багш О. БАЯРЦЭЦЭГ
Понарамалық сабақ.
Solving Equations 3x+7 –7 13 –7 =.
Pythagoras Theorem Example
,, 'III \-\-
Print out label on Drill 2mm holes for magnets
Presentation transcript:

“Amplitude Cooling” in Step III & IV Timothy Carlisle

from CM28

Step III Empty 10mm  Pz = 1 MeV/c Step IV Empty 10mm  Pz = 1 MeV/c Amp Cut [mm] NN NN Amp OUT [mm] Amp IN [mm] Amp OUT [mm] Amp IN [mm] cooling

Step III LiH 10mm  Pz = 1 MeV/c Step IV LH2 10mm  Pz = 1 MeV/c Amp Cut [mm] NN NN Amp OUT [mm] Amp IN [mm] Amp OUT [mm] Amp IN [mm] cooling

An Aside: Step VI Amp OUT [mm] Amp IN [mm] (Note: 10x less events than III / IV ) Amp Cut [mm] NN 1000mu 10mm  Pz = 1 MeV/c

Amp Cut = 30mm Amp Cut = 60mm Amp Cut = 80mm  in  out /N Total cooling Input Emittance [mm]  in  out /N Total