F March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.1 Saturday Morning Physics - Accelerators Accelerators What’s Up Now? What’s Up.

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Presentation transcript:

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.1 Saturday Morning Physics - Accelerators Accelerators What’s Up Now? What’s Up Next? <<<< We Are Here...

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.2 Accelerators - What’s Up Next? What Up Next? –electrons and positrons : e + e - Colliding Beams –protons and protons : pp Colliding Beams –muons and muons :  +  - Colliding Beams –neutrino beam : From decaying muons But first, a word about recent times...

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.3 Recent Times... Physics Today January 2001 –Maury Tigner (Cornell University) Comparing hadrons and leptons –Constituent hadron collision energy is about 1/10 of total hadron beam energies –Constituent lepton collision energy is all of total lepton beam energies Leveling off? … yes … why? –It’s a fact of life if you keep using the same concepts and evolve with the same basic technology Constituent Collision Energy (GeV) Year of Collisions

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.4 e + e - Linear Colliders The good new is: –The electron is a lepton A point (so far as we can see) Simple particles give simpler interactions –Precision tool (if you know where to look) –Q4: How is it that we see more matter than antimatter? –Q2: How does it all behave? The bad new is: –Not much mass … radiates photons like crazy when you deflect them

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.5 NLC is an e+e- option Insert NLC Stick diagram from Word File NLC = Next Linear Collider

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.6 Schematic of NLC RF Test Fermilab is developing a plan for performing this test in a recycled fixed target beam enclosure … see next slides NLC RF Test = ETF

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.7 A Tunnel for an NLC RF Test The ETF ceclosure is mostly empty now … and that is good!

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.8 And Building for an NLC RF Test The MP9 building is now being used to make parts of the CMS detector for the LHC … but it can be reused for the ETF.

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide meter long NLC RF structure Made by the KEK lab in Japan and tested at the SLAC lab in California Each structure has 206 disks … see next slide

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.10 NLC RF copper disks Each disk has a 61 mm diameter and 8 mm thickness. The electron or positron beam goes through the center hole and unwanted energy is taken away in the four side channels.

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.11 NLC Permanent Magnet Insert Shunt Quad on SSW stand by Volk

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.12 TESLA at DESY is also an e+e- Option TESLA = TeV Electron Superconducting Linear Accelerator The DESY lab is proposing an e+e- collider. The accelerator is made of superconducting rf cavities. The tunnel is about 6 meters in diameter.

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.13 Protons on protons The good news is: –We know how to do this … standard techniques –This gives us the energy frontier –This is the path to discovery –Q1: What’s it all made of? –Q2: How does it all behave? The bad news is: –Continuing the standard approach costs too much

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.14 LHC IR Quadrupole Magnet Cold Mass Only Insert P. Schlabach’s Slide … ASC 18 Sep 2000 … Slide 3

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.15 LHC IR Quadrupole Magnet Fermilab is making several high gradient quadrupole magnets for the Interaction Regions at the LHC This quadrupole magnet is 36 inches in diameter and about 7 meters long

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.16 VLHC - Low Field Option G.W. Foster and V. Kashikhin May 2000

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.17 VLHC - Low Field Option G.W. Foster and V. Kashikhin May 2000

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.18 VLHC - Low Field Option G.W. Foster and V. Kashikhin May 2000

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.19 A Tunnel Vision for the VLHC The low field is on the bottom, the high field is on the top. The high and low field are shown in the LEP tunnel as an example. The tunnel is real and is about 12 feet in diameter.

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.20 Insert Ernie’s “Comments on a … vlhc”

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.21 Insert Ernie’s “500 km pipetron map study”

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.22 Muons on muons The good news is: –Just another simple lepton … just like the electron –But heavier than the electron They don’t radiate photons like crazy They interact better (40,000 times better) with Higgs –Q3: How do particles come by their mass? The bad new is: –They only stay around for seconds (or so) –They spit out electrons … which then radiate like crazy

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.23 Insert Muon Collider Schematic from Word

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.24 Neutrino Beam The good new is: –All the muons decay to electrons and neutrinos –Never been done … surprises probably in store –Q1, Q2, Q3, Q4, Q4++ The bad news is: Not discovery, not simple … So, maybe not “interesting”? Aside: Really global-sized experiments

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.25 Insert DF slide with “NF at Fermilab”

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.26 Insert MuSR FESS Slide with Geology

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.27 Insert Geer L/E and other Physics Guidance

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.28 And Into the Beyond... The good new and the bad new is: –Hasn’t been done before … –For good reasons, usually... One example is Plasma acceleration –100 TeV center of mass … and... –All the equipment fits on the Fermilab site –But is costs too much to operate … –At least … using today’s technology

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.29 Insert Linda’s “Plasma acceleration”

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.30 A0 Photoinjector at Fermilab RF Gun and focussing solenoids

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.31 A0 Photoinjector at Fermilab Spectrometer magnets, plasma chamber, and beam dump

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.32 Summary This is still fun. –Q1: So what IS it all made of? and –Q2: How DOES it all behave? etc etc There is still lots to do. –Decades (in performance and on calendars) –The best ideas are yet to come...

f March 31, 2001David Finley / Fermilab Saturday Morning Physics Slide 2.33 Behind the... (not likely on SHOW AIRS: SAT 3/31 at 9am CT Your Host: David Finley Fermilab Accelerators SCIENCE