Physics class schedule

Here is what I can gather about our UniGe schedule. The E/M was sent out by Prof Pohl. The QM I got from the agenda book which I assume is right. I also assume that the Tuesday class is the lecture. My guess is that there will be an English discussion for QM also (hopefully).

M: 10-12noon E/M lecture (main auditorium in Ecole de physique)
2-3pm E/M discussion in English (DPNC Library Room 211 in Ecole de physique )
T: 10-12noon QM
W: 4-6pm QM
T: 10-12noon QM
F: 2-4pm E/M discussion (lecture hall A50B in Science I)

I’ll update it as we get more info. Classes start Feb 22nd.
-Andrea

Outcome from Chamonix: Better in the long run

Last week, the Chamonix workshop once again proved its worth as a place where all the stakeholders in the LHC can come together, take difficult decisions and reach a consensus on important issues for the future of particle physics. The most important decision we reached last week is to run the LHC for 18 to 24 months at a collision energy of 7 TeV (3.5 TeV per beam). After that, we’ll go into a long shutdown in which we’ll do all the necessary work to allow us to reach the LHC’s design collision energy of 14 TeV for the next run. This means that when beams go back into the LHC later this month, we’ll be entering the longest phase of accelerator operation in CERN’s history, scheduled to take us into summer or autumn 2011.

What led us to this conclusion? Firstly, the LHC is unlike any previous CERN machine. Because it is a cryogenic facility, each run is accompanied by lengthy cool-down and warm-up phases. For that reason, CERN’s traditional ‘run through summer and shutdown for winter’ operational model had already been brought into question. Furthermore, we’ve known for some time that work is needed to prepare the LHC for running at energies significantly higher than the 7 TeV collision energy we’ve chosen for the first physics run. The latest data show that while we can run the LHC at 7 TeV without risk to the machine, running it at higher energy would require more work in the tunnel. These facts led us to a simple choice: run for a few months now and programme successive short shutdowns to step up in energy, or run for a long time now and schedule a single long shutdown before allowing 14 TeV (7 TeV per beam).

A long run now is the right decision for the LHC and for the experiments. It gives the machine people the time necessary to prepare carefully for the work that’s needed before allowing 14 TeV. And for the experiments, 18 to 24 months will bring enough data across all the potential discovery areas to firmly establish the LHC as the world’s foremost facility for high-energy particle physics.

I’d like to invite you all to the summary of the Chamonix workshop on Friday 5 February at 14:00 in the Main auditorium. See:
http://indico.cern.ch/conferenceDisplay.py?confId=83135

Steve Myers
Director for Accelerators and Technology

From link

About Poisson Distribution…

I found out that Poisson distribution “expresses the probability of a number of events occurring in a fixed period of time if these events occur with a known average rate and independently of the time since the last event.” (wiki) I think it may be related to QM.

Anyways, the only parameter λ in the poisson equation is “expected number of occurrences” in a given interval; that is, if λ is set to be 1, the event is expected to happen only one time in a given interval (time/distance/whatever). Because λ is always positive, the poisson equation is always larger than 0, and thus the negative part can be thrown out…(maybe?)

From the wiki, the plot shows that, in the case of λ=1, the probability of the event to occur exactly (shown by the x-axis) is about 0.7 (which is about the same as the plot I got from fitting). [But I don’t fully understand why…] As λ increases, the plot spreads out. (Why? – I am still thinking …)

Anyways, I just share what I know and what I don’t know… If I said something wrong/you know something that I miss, let me know!

Thanks,

Elim =D

Talk on Dark Matter…

Hey all!

So I mention this to a few of you already, but Hidefumi Tomita is giving a talk during a Photon meeting tomorrow. The title of his talk is “Detector Development for Direction-Sensitive Dark Matter Research”. Some of you expressed interest on seeing this and I am currently working with Jess and Ryan about setting up a webchat/Skype so we can listen to the talk too. Photon starts at 5pm (so 11pm here). I know you all probably have better things to do with your Friday evenings but if anyone is interested, come down to our room (Elim, Chelsea and I are in #33) maybe a few minutes to 11pm.

They plan for the talk to be 30 mins so it will definitely be over by midnight.

We will also get to say hi to our Boston friends! Let me know if you are interested in coming! (I will buy some sort of snack for us all if I am feeling generous at the time?)

-Andrea

Somewhat helpful tutorial….

Hey all!

When I started using ROOT over the summer, there was this Tutorial I found… online (not the CERN one, it’s actually by Professor Bose) which I thought was very helpful for basic histogram stuff. I know some of you have been asking how to use ROOT besides just opening files and this may be beneath what some of you know already, but just in case….

(This is also me testing to see if posting things works…)

Hope this helps! 🙂

-Andrea