Simulation Plan Discussion What are the priorities? – Higgs Factory? – 3-6 TeV energy frontier machine? What detector variants? – Basic detector would.

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Presentation transcript:

Simulation Plan Discussion What are the priorities? – Higgs Factory? – 3-6 TeV energy frontier machine? What detector variants? – Basic detector would look fairly similar – Would begin with SiD tracker layout, but with CMS phase 2 tracker modules (1mm x 100 micron) and mass (CO 2 cooling) – Calorimeter is more difficult – need to study timing effects on jet energy resolution Dual readout option Pixelated option Study background mitigation for one option R. Lipton Higgs Factory Workshop[ 11/16/2012 1

Rates Overall rates Luminosity estimates are in the range If we fold a 4.2 MeV Breit- Wigner with a 2.5 MeV Gaussian beam we get a on-peak cross section of ~46 pb This gives us between 3,000 (5 MeV, ) and 46,000 (2.5 MeV, ) Higgs/year The physics we can do depends strongly on machine parameters R. Lipton Higgs Factory Workshop[ 11/16/ Cross section At scan point

Width Fitting Results (Han and Liu) ILC Expectations (Archive ) Int. Lum fb -1 ILC ~ 50 MeVILC ~ 5 MeV R. Lipton Higgs Factory Workshop[ 11/16/2012 3

Further Work The Han and Liu results provide an nice framework for future studies – the essential elements are there but we need to access the reach with realistic detector and background simulation What is the b-tag efficiency with background? What are the dominant backgrounds to WW*? – Han and Liu assume unit efficiency and no  /Z* background – What calorimetery is needed for the WW*->4-jet mode? How does adding background affect the studies? R. Lipton Higgs Factory Workshop[ 11/16/2012 4

Detector Simulation Initial work based on ILCROOT – moving to LCSIM Both full and fast simulation available – Mars backgrounds incorporated into full simulation – A variety of detector options can be explored MARS particles handed off to LCSIM at detector boundries Background only studies – Full event simulation Use timing to cut off tracing of “late” particles Study parameterization of backgrounds Build background library – Background characteristics Time and energy distributions R. Lipton Higgs Factory Workshop[ 11/16/2012 5

Timing In a Tracker There is already an example of a fast timing IC design at CERN for CMS upgrades Intent is to use fast timing to reject “loopers” 65 nm process – Pixel ~ 1mm x 100  x 200  thick – Peaking time: 6 ns – 220 e- ENC for 260 fF input capacitance – Consumption for nominal bias: 65 uA Jitter for 0.6fC V th and 2.5fC signal; ~50 ps rms Jitter for 1 fC signal; ~100 ps rms. Time resolution defined by time walk (~3 ns)  without correction the resolution will be ~500 ps RMS Time walk for signals 1 to 10 fC (0.6 fC threshold) ; <3 ns R. Lipton Higgs Factory Workshop[ 11/16/2012 6

Bottom View ROIC Readout bus Foam spacer Foam spacer Analog Flex Circuit Foam spacer Pixelated two layer trigger module for CMS ~ 1.1% RL

Vertex Detector ILC inner radius ~1.5 cm set by beamstrahlung MuC Inner radius ~5 cm set by EM background from cone Preserve IP resolution by scaling by r outer /r inner MuC vertex ILC vertex ILC Charged particle Density vs radius (Mazzacane) R. Lipton Higgs Factory Workshop[ 11/16/2012 9

Higgs Plans Fast simulation studies of Higgs width measurements – Develop optimized sets of algorithms to measure Higgs mass and width with realistic jet and tracker resolutions. Develop MARS background model suitable to 125 GeV Full simulation with background included – Verify that high purity tracking can be achieved – Understand jet energy resolutions with timing cuts. – Redo the fast simulation studies with fully simulated backgrounds Longer term focus is on a high energy machine – that is the natural path for a MUC Higgs Factory Much of the development will apply to both R. Lipton Higgs Factory Workshop[ 11/16/

Higgs vs 3 TeV Higgs studies will be of significant interest for the Snowmass process – Physics is unique – initial studies can use fast simulation Physics of 3-6 TeV machine is very similar to e + e - - already covered by CLIC study – Make the case that backgrounds can be handled – Quantify tradeoffs due to fast timing and radiation hardness “Generic” study of background mitigation – use HE machine (we have the simulation now) – Add comparison of 125 GeV background when available R. Lipton Higgs Factory Workshop[ 11/16/