First successful beam at record energy of 6.5 TeV
home.web.cern.ch
home.web.cern.ch
I highly recommend 'Particle Fever', in case you haven't seen it yet. It cover's the LHC before the shutdown and restart, which included the Higgs boson discovery. Just fascinating look into what an international collaboration of human beings can accomplish.
IMDB: http://www.imdb.com/title/tt1385956/
Trailer: https://www.youtube.com/watch?v=Rikc7foqvRI
Netflix: http://www.netflix.com/WiMovie/70296323?trkid=13752289
BIG-BANG-BELIEVING-BABBLERS
dead darkness drool that drips from the drooping face
Every fickle frame is filled with the foul stench of arrogant atheists
sad little men sit in the silent abyss of spiritual darkness wearing their dirty diapers of despair
dead-dogma doctrines
best movie ever, could use moar magnets
Though now as I go back through, some of the more ridiculous comments seem to be disappearing...
http://op-webtools.web.cern.ch/op-webtools/vistar/vistars.ph...
all the changing numbers are actually dynamically generated PNG's...
Yes: there's a link called "Doc" on the bottom of the page. This is the one for LHC Page 1, which is the most important display: http://op-webtools.web.cern.ch/op-webtools/vistar/Doc/LHC1.p...
No: well, you may only understand it if you have some background knowledge in some particle physics terms.
For finer detail of discovery, we need more and more power in the accelerator.
TLDR: Hopefully opening the door for some mind blowing discoveries.
Basically, energy and mass are interchangeable in some violent reactions (like the ones at the LHC or that released in atomic explosions) as we know because of Einstein. This means that as we increase the energy of these violent collisions, the more energy that is available to be converted into the mass of possible particle products.
It should be noted that it isn't like we add mass to the products like adding snow to a snow ball, it isn't a continuum. It's more like a threshold. If a particle has a mass of 938 MeV, say, we will see it in a collision as a product only if s for that interaction is greater than 938 MeV. In fact, it must be a bit larger than this, because while some energy gets converted to mass, some energy also needs to get converted to energy of motion for these products too. Otherwise, they won't reach our the detectors in our apparatus for us even to see them.
We haven't seen a number of massive particles we think should exist, from a theory called "Supersymmetry". Note that we do not really know from theory what these masses should be, but we need them to exist for our current models of the universe. Our current guess then for why we don't see them is that we just haven't passed their threshold masses sufficiently to create them first and with enough energy after in order to see them.
That's why 6.5 TeV which implies a max s of 13 TeV is important. It's like we've increased the range of our "scan" of particle masses. It means we'll produce more massive particles (if they exist) and more of them in number with sufficient energy to actually see them.
One of my favorite videos on this topic was a Great Courses video by Sean Carroll. Well worth the $40. http://www.thegreatcourses.com/courses/the-higgs-boson-and-b...
https://www.youtube.com/playlist?list=PLpH1IDQEoE8Q8842yVe-V...
It goes into a little more detail than a typical popularizing course, but enough even for laypeople to understand.
David Butler also has a great introduction to astronomy in the same style:
https://www.youtube.com/playlist?list=PLpH1IDQEoE8QWWTnWG5cK...
Just as a comment, we "only" saw the Higgs Boson (around 125GeV) at LHC energy levels, so the Higgs might get produced at small collision energies, but with a much lower probability
(I'm not disagreeing with you btw)
edit: did some Googling and found some documentation (https://en.wikipedia.org/wiki/Safety_of_high-energy_particle...). It cites an estimated upper limit of 1 in 50 million and references the book in which that estimate is made.
A black hole is no different than any other massive object in that it doesn't exert any stronger pull than its mass allows for. In other words, if the Sun suddenly turned into a black hole right now, we would not get "sucked" into it. The Earth would continue orbiting at the same period and distance. Of course, it would suck (no pun intended) not to have sunlight but hey, maybe the energy emitted by the accretion disc would equal the energy output of the sun :P! Of course, an accretion disc would probably take a while to form, so we would probably be fucked anyway, but certainly not because we would be sucked into the black hole.
Similarly, if the LHC created a black hole through its collisions, I can't see how it would be that massive. If it's not very massive, then it's not a threat. In fact, there are theories that support the notion that it would evaporate rather quickly (via Hawking radiation). Of course, I don't have any numbers on this and only have a laymen's knowledge of the physics involved. Anyone care to comment with more info?
(I don't think I have an interesting opinion when it comes to the question of whether such a hole would evaporate or not, but the question of why having a blackhole on the surface of the planet is bad is easier to think about)
The article ufmace links in a sibling thread addresses the issue more directly, it wouldn't grow fast enough to be something to worry about, thousands of years is the wrong time scale.
I know what you mean, but I still think you have to look at the numbers. It seems plausible to me that the black hole might be so small that it would take literally millions of years or more to consume enough mass to become a threat. And that might even depend a lot on chance since most particles would just drift by it without passing inside of its event horizon since the force of gravity has very little effect at those scales.
http://en.wikipedia.org/wiki/Cosmic_ray#/media/File:Cosmic_r...
Let's move beyond "seems plausible" and try to work with "supported by the data".
Far higher energy stuff than anything we can dream of producing in a lab happens all over the world all the time. And the stuff that's documented now is only the things that have happened since we started being able to detect and measure it.
https://medium.com/starts-with-a-bang/could-the-lhc-make-an-...
TL:DR: 1.) If these miniature black holes exist, the Earth has been getting hit by them for billions of years, and it’s still here. 2.) If you do create a miniature black hole, they will decay, via Hawking Radiation, on ridiculously small timescales. 3.) You can compute the rate at which a black hole eats matter, and it’s not even close to being as small as the lifetime of our planet
Thanks for the wonderful article.
A small question. Is this rate of consumption linear? Correct me if I'm wrong, the heavier the black hole gets, more and faster it can absorb matter. Of course given there is matter around it.
The article author calculated how big that would be, and the black hole would reportedly need to accumulate about a billion tons of mass before it could start to grow exponentially.
Very small black holes are not stable. For all we know, they are being created all the time, but they evaporate almost immediately.
Sources and half-assed math: http://en.wikipedia.org/wiki/Ultra-high-energy_cosmic_ray
Lower limit for UHE cosmic ray: 10^19 eV
10^19 eV / 13 TeV = 769 230.769
24 events detected / 3 years in an area of 3,000 sq. km
Surface area of the Earth = 510 million sq. km
(510.1 million / 3000) * (27 / (3 years)) * 24 hours = 4188 events per day, or 7.19241 × 10^15 in 4.7 billion years.
Or rather, irrelevant if it does happen. You work out the mass loss via Hawking radiation, it's high enough at those mass levels that they'd just go "poof". The Earth isn't dense enough to sustain such a black hole.
Not to mention that if the LHC produced said micro black holes, they'd be produced by cosmic rays anyways.
In particle physics there are a couple important fundamental principles, one of the most basic is the various conservation rules. Energy/mass, charge, lepton number, baryon number, etc, all of these things are conserved. But that leaves open a big window, because it means you can have any sort of particle reaction possible as long as you have enough energy and the various other "quantum numbers" (charge, leptons, whatever) are balanced. So, for example, if you have nothing more than high energy photons (gamma rays) you can create particle/anti-particle pairs easily (such as electrons/positrons) because in those situations everything that should be conserved is exactly balanced (since anti-particles have opposite charge, spin, lepton number, and so on). You can get more complex particle reactions so long as they are still balanced.
Now, let's say you want to study a particular particle. If those particles aren't naturally occurring, like protons or neutrons or electrons, then you'll need to figure out how to create them. And that means creating conditions where there's more energy available than the energy required for reactions that involve those particles. For example, the LHC was operating at 7 TeV total energy for collisions, which enabled them to discover the 125 GeV Higgs boson. Note that there's a significant difference in those energy levels (nearly a factor of 100), and this is because the process is somewhat inefficient and random and also there's some overhead in the reactions. For example, you need twice the energy of an electron particle in order to see electron-positron creation reactions, due to that balancing aspect.
Ultimately what you have is a huge collection of reactions due to particle collisions at a given energy level. And these reactions can be compared against the reactions you'd expect to see. With more energy in the collisions you push out the "search space" into different realms involving different particles and different phenomena. You can then use that data to perform "tests", by comparing what you actually see to what you'd expect to see given certain theories (such as the Higgs-mechanism theory), and in that way verify or falsify a theory. The more energy you have the easier it is to search for higher energy particles and phenomena.
The LHC energy boost will make it possible to explore new realms of physics. To either rule out the existence of potential particles at certain mass levels or to establish their existence, as with the Higgs-boson. It'll make it possible to narrow down some constraints on the Higgs-mechanism theory as well as potentially fill in some details (or rule out some possibilities) with regard to Dark Matter.
http://www.nature.com/polopoly_fs/1.17081!/menu/main/topColu...
When LHC is running in full, a total of 2808 bunches per beam are expected to be colliding there. That's a lot of energy.
Maybe next year the energy will be increased to 7 TeV.
At first I wondered if it were this (Another World intro, 1991): https://www.youtube.com/watch?v=1j4gO9sR7zs
That game looks priceless. I'll have to play it. Thanks for the video :)
The coordination of the control signals is quite fun: it is capable of synchronizing events tens of kilometers apart to nanosecond accuracy.