Rolling in the Higgs
๐ต 1190 characters
โฑ๏ธ 3:46 duration
๐ ID: 15007202
๐ Lyrics
There's a collider under Geneva
Reaching new energies that we've never achieved before
Finally we can see with this machine
A brand new data peak at 125 GeV
See how gluons and vector bosons fuse
Muons and gamma rays emerge from something new
There's a collider under Geneva
Making one particle that we've never seen before
The complex scalar
Elusive boson
Escaped detection by the LEP and Tevatron
The complex scalar
What is its purpose?
It's got me thinking
We could have had a model (Particle breakthrough, at the LHC)
Without a scalar field (5-sigma result, could it be the Higgs)
But symmetry requires no mass (Particle breakthrough, at the LHC)
So we break it, with the Higgs (5-sigma result, could it be the Higgs)
Baby I have a theory to be told
The standard model used to discover our quantum world
SU(3), U(1), SU(2)'s our gauge
Make a transform and the equations shouldn't change
The particles then must all be massless
Cause mass terms vary under gauge transformation
The one solution is spontaneous
Symmetry breaking
Roll your vacuum to minimum potential
Break your SU(2) down to massless modes
Into mass terms of gauge bosons they go
Fermions sink in like skiers into snow
Reaching new energies that we've never achieved before
Finally we can see with this machine
A brand new data peak at 125 GeV
See how gluons and vector bosons fuse
Muons and gamma rays emerge from something new
There's a collider under Geneva
Making one particle that we've never seen before
The complex scalar
Elusive boson
Escaped detection by the LEP and Tevatron
The complex scalar
What is its purpose?
It's got me thinking
We could have had a model (Particle breakthrough, at the LHC)
Without a scalar field (5-sigma result, could it be the Higgs)
But symmetry requires no mass (Particle breakthrough, at the LHC)
So we break it, with the Higgs (5-sigma result, could it be the Higgs)
Baby I have a theory to be told
The standard model used to discover our quantum world
SU(3), U(1), SU(2)'s our gauge
Make a transform and the equations shouldn't change
The particles then must all be massless
Cause mass terms vary under gauge transformation
The one solution is spontaneous
Symmetry breaking
Roll your vacuum to minimum potential
Break your SU(2) down to massless modes
Into mass terms of gauge bosons they go
Fermions sink in like skiers into snow
โฑ๏ธ Synced Lyrics
[00:04.28] There's a collider under Geneva
[00:09.27] Reaching new energies that we've never achieved before
[00:13.76] Finally we can see with this machine
[00:18.36] A brand new data peak at 125 GeV
[00:22.57] See how gluons and vector bosons fuse
[00:26.75] Muons and gamma rays emerge from something new
[00:31.66] There's a collider under Geneva
[00:36.23] Making one particle that we've never seen before
[00:41.50] The complex scalar
[00:44.53] Elusive boson
[00:46.75] Escaped detection by the LEP and Tevatron
[00:51.04] The complex scalar
[00:53.78] What is its purpose?
[00:55.84] It's got me thinking
[00:58.03] We could have had a model (Particle breakthrough, at the LHC)
[01:02.55] Without a scalar field (5-sigma result, could it be the Higgs)
[01:07.11] But symmetry requires no mass (Particle breakthrough, at the LHC)
[01:12.69] So we break it, with the Higgs (5-sigma result, could it be the Higgs)
[01:16.98] Baby I have a theory to be told
[01:22.83] The standard model used to discover our quantum world
[01:27.13] SU(3), U(1), SU(2)'s our gauge
[01:31.33] Make a transform and the equations shouldn't change
[01:35.62] The particles then must all be massless
[01:41.90] Cause mass terms vary under gauge transformation
[01:46.01] The one solution is spontaneous
[01:50.73] Symmetry breaking
[01:53.27] Roll your vacuum to minimum potential
[02:34.96] Break your SU(2) down to massless modes
[02:40.13] Into mass terms of gauge bosons they go
[02:44.72] Fermions sink in like skiers into snow
[02:56.09]
[00:09.27] Reaching new energies that we've never achieved before
[00:13.76] Finally we can see with this machine
[00:18.36] A brand new data peak at 125 GeV
[00:22.57] See how gluons and vector bosons fuse
[00:26.75] Muons and gamma rays emerge from something new
[00:31.66] There's a collider under Geneva
[00:36.23] Making one particle that we've never seen before
[00:41.50] The complex scalar
[00:44.53] Elusive boson
[00:46.75] Escaped detection by the LEP and Tevatron
[00:51.04] The complex scalar
[00:53.78] What is its purpose?
[00:55.84] It's got me thinking
[00:58.03] We could have had a model (Particle breakthrough, at the LHC)
[01:02.55] Without a scalar field (5-sigma result, could it be the Higgs)
[01:07.11] But symmetry requires no mass (Particle breakthrough, at the LHC)
[01:12.69] So we break it, with the Higgs (5-sigma result, could it be the Higgs)
[01:16.98] Baby I have a theory to be told
[01:22.83] The standard model used to discover our quantum world
[01:27.13] SU(3), U(1), SU(2)'s our gauge
[01:31.33] Make a transform and the equations shouldn't change
[01:35.62] The particles then must all be massless
[01:41.90] Cause mass terms vary under gauge transformation
[01:46.01] The one solution is spontaneous
[01:50.73] Symmetry breaking
[01:53.27] Roll your vacuum to minimum potential
[02:34.96] Break your SU(2) down to massless modes
[02:40.13] Into mass terms of gauge bosons they go
[02:44.72] Fermions sink in like skiers into snow
[02:56.09]