diff --git a/html/BBbar.html b/html/BBbar.html index 28cf930..59958b5 100644 --- a/html/BBbar.html +++ b/html/BBbar.html @@ -1,6 +1,6 @@

You discovered the Oscillation of Neutral B Mesons.

The Oscillation of Neutral B mesons
-A plot from one of the original publications +

More information will come soon...

diff --git a/html/CPV.html b/html/CPV.html index 9ce8164..056104c 100644 --- a/html/CPV.html +++ b/html/CPV.html @@ -12,7 +12,7 @@ It turned out that this is wrong, as was discovered by Cronin, Fitch et al. in 1
CPV in the Kaon System
- A plot from the original publication + A plot from the original publication

In 1964, Cronin, Fitch, et al. showed that CP symmetry is broken in the decay of the long-lived neutral K meson.

diff --git a/html/H.html b/html/H.html index fa158fe..a3ac319 100644 --- a/html/H.html +++ b/html/H.html @@ -1,6 +1,6 @@

You discovered the Higgs-boson.

The Higgs boson
-A plot from one of the original publications +

More information will come soon...

diff --git a/html/Jpsi.html b/html/Jpsi.html index ccb4b0e..e8b392b 100644 --- a/html/Jpsi.html +++ b/html/Jpsi.html @@ -1,6 +1,6 @@

You discovered the J/ψ meson!

The J/ψ meson
-A plot from one of the original publications +A plot from one of the original publications

The J/ψ is a meson consisting of a charm quark and its antiquark. It is the first excited state of the charmonium (a bound charm-anticharm state), and was discovered independently by two research groups in 1974: one at the Stanford Linear Accelerator Center, led by Burton Richter, and one at the Brookhaven National Laboratory, led by Samuel Ting of MIT. Richter and Ting were awarded the 1976 Nobel Prize in Physics for their shared discovery.

diff --git a/html/antihydrogen.html b/html/antihydrogen.html index f771694..2f82688 100644 --- a/html/antihydrogen.html +++ b/html/antihydrogen.html @@ -1,6 +1,5 @@

You discovered Antihydrogen.

The antihidrogen
-A plot from one of the original publications

More information will come soon...

diff --git a/html/b.html b/html/b.html index b8475b2..3196f51 100644 --- a/html/b.html +++ b/html/b.html @@ -1,7 +1,7 @@

You discovered the bottom quark!

The bottom (or beauty) quark
-A plot from one of the original publications +A plot from one of the original publications

The bottom (or beauty) quark is a third-generation quark with a charge of −⅓. It has a large mass (around 4.2 GeV/c2 — more that four times the mass of a proton!). The bottom quark is notable because it is a product in almost all decays of the top quark and is a frequent decay product for the Higgs boson. diff --git a/html/tau.html b/html/tau.html index fe62500..a32439d 100644 --- a/html/tau.html +++ b/html/tau.html @@ -1,6 +1,6 @@

You discovered the τ lepton!

The τ lepton
-A plot from the original publication +A plot from the original publication

The τ (tau) is an elementary particle that can be thought of as a much heavier cousin of the electron, with a spin of ½. It belongs to the family of leptons, along with the electron, the muon, and the three neutrinos. Despite the origin of the word lepton (meaning fine, small, thin) the τ is very massive at 1776.82 MeV/c2, which is nearly 3500 times the mass of the electron and around twice the mass of the proton.

diff --git a/html/top.html b/html/top.html index 370ec48..ff4dcec 100644 --- a/html/top.html +++ b/html/top.html @@ -1,6 +1,6 @@

You discovered the top quark!

The top quark
-A proton and an antiproton annhilate to form a top-antitop pair +A proton and an antiproton annhilate to form a top-antitop pair

At 174.2 GeV/c2, the top quark is the heaviest particle we know of. It belongs to the third generation of quarks and has a charge of ⅔. As a result of its large mass, it decays (mostly into bottom quarks) almost instantly after it is produced. This behemoth does not form bound states with other quarks or antiquarks. diff --git a/html/weak.html b/html/weak.html index 7a6d2d4..d06adff 100644 --- a/html/weak.html +++ b/html/weak.html @@ -1,6 +1,6 @@

You discovered the W and Z bosons!

The weak force
-A W− boson produced in the transformation of a neutron into a proton +A W− boson produced in the transformation of a neutron into a proton

The weak interaction is a nuclear process that is responsible, among other things, for β (beta) decay the transformation of neutrons into protons. The weak force is mediated by two bosons called the W and the Z. The W comes in two types: W+ and W−. The Z is neutral and is sometimes represented as Z0.