Chords for Rolling in the Higgs (Adele Parody) | A Capella Science
Tempo:
105.05 bpm
Chords used:
G
F
Am
A
E
Tuning:Standard Tuning (EADGBE)Capo:+0fret
Start Jamming...
[Am]
[A] There's a collider [B] under Geneva
[G] Reaching new energies that we've never achieved [D] before
[A] Finally we [B] can see with this machine
[G] A brand new data peak at 125 GeV
[D] See [E] how gluons [B] and vector bosons fuse
[G] Muons and gamma rays emerge from something [D] new
[A] There's a [E] collider under [B] Geneva
[G] Making one particle that we've never seen before
[F] A [G] complex scalar elusive [Em] boson
Escaped [F] detection by the lepantevatron
The [G] complex scalar, what [Em] is its purpose?
It's got me [E] thinking
We could have had [Am] a model
[G] Without a scalar [F] field
But [G] symmetry [A] requires [Am] a new [G] mass
So we [F] break it up with the heat
[G]
[A] Baby, I have [E] a theory to be told
[G] A standard model used to discover our quantum world
[A] [E] SU3U1 SU2's our gauge
[G] Make gauge transform and the equations should have changed
[F] The particle [G] goes and must all [Em] be massless
Because mass [F] terms vary under gauge transformation
The one [G] solution is [Em] spontaneous
See a symmetry break [F] it
We could have had [Am] a model
[G] Without a scalar [F] field
[G] But symmetry [A] requires [Am] a [G] new mass
So we [F] break it up with the heat
[G] Could have had [F] a model
[G] Without a [Am] scalar field
[G] But symmetry [F] requires a new mass
So we [G] break it up with the heat
Grow your vacuum to minimal [Am] potential
Break your [Bb] SU2 down to massless moles
Into mass terms of gauge bosons they go
For [A] me I'm sinking like gears [G] into stars
[Am] [G] We could have had [F] a model
[G] We could have had [Am] a model
[G]
[F] Model, model, model
[G] We could have [Am] had a model
[G] Without a scalar [F] field
[G] But symmetry [Am] requires a new [G] mass
So we [F] break it up with the [G] heat
Could have [Am] had a model
[G] Without a [F] scalar field
[G] But symmetry [Am] requires a new [G] mass
So we [F] break it up with the heat
[G]
Acapella Science
[A] There's a collider [B] under Geneva
[G] Reaching new energies that we've never achieved [D] before
[A] Finally we [B] can see with this machine
[G] A brand new data peak at 125 GeV
[D] See [E] how gluons [B] and vector bosons fuse
[G] Muons and gamma rays emerge from something [D] new
[A] There's a [E] collider under [B] Geneva
[G] Making one particle that we've never seen before
[F] A [G] complex scalar elusive [Em] boson
Escaped [F] detection by the lepantevatron
The [G] complex scalar, what [Em] is its purpose?
It's got me [E] thinking
We could have had [Am] a model
[G] Without a scalar [F] field
But [G] symmetry [A] requires [Am] a new [G] mass
So we [F] break it up with the heat
[G]
[A] Baby, I have [E] a theory to be told
[G] A standard model used to discover our quantum world
[A] [E] SU3U1 SU2's our gauge
[G] Make gauge transform and the equations should have changed
[F] The particle [G] goes and must all [Em] be massless
Because mass [F] terms vary under gauge transformation
The one [G] solution is [Em] spontaneous
See a symmetry break [F] it
We could have had [Am] a model
[G] Without a scalar [F] field
[G] But symmetry [A] requires [Am] a [G] new mass
So we [F] break it up with the heat
[G] Could have had [F] a model
[G] Without a [Am] scalar field
[G] But symmetry [F] requires a new mass
So we [G] break it up with the heat
Grow your vacuum to minimal [Am] potential
Break your [Bb] SU2 down to massless moles
Into mass terms of gauge bosons they go
For [A] me I'm sinking like gears [G] into stars
[Am] [G] We could have had [F] a model
[G] We could have had [Am] a model
[G]
[F] Model, model, model
[G] We could have [Am] had a model
[G] Without a scalar [F] field
[G] But symmetry [Am] requires a new [G] mass
So we [F] break it up with the [G] heat
Could have [Am] had a model
[G] Without a [F] scalar field
[G] But symmetry [Am] requires a new [G] mass
So we [F] break it up with the heat
[G]
Acapella Science
Key:
G
F
Am
A
E
G
F
Am
[Am] _ _ _ _ _ _ _ _
[A] There's a collider [B] under Geneva _
[G] Reaching new energies that we've never achieved [D] before
[A] Finally we [B] can see with this machine
[G] A brand new data peak at 125 GeV
[D] See [E] how gluons [B] and vector bosons fuse _
[G] Muons and gamma rays emerge from something [D] new
[A] There's a [E] collider under [B] Geneva _
[G] Making one particle that we've never seen before
[F] A _ [G] complex scalar elusive [Em] boson
Escaped [F] detection by the _ lepantevatron
The [G] complex scalar, what [Em] is its purpose?
It's got me [E] thinking
We could have had [Am] a model
_ _ [G] _ Without a scalar [F] _ _ field
But [G] symmetry [A] requires [Am] a new [G] mass
So we [F] break it up with the heat
[G] _ _
[A] Baby, I have [E] a theory to be told
[G] A standard model used to discover our quantum world _
[A] _ _ _ [E] SU3U1 SU2's our gauge
[G] Make gauge transform and the equations should have changed
[F] _ The particle [G] goes and must all [Em] be massless
Because mass [F] terms vary under gauge transformation
The one [G] solution is [Em] spontaneous
See a symmetry break [F] it
We could have had [Am] a model
_ _ [G] _ Without a scalar [F] field
_ _ _ _ [G] But symmetry [A] requires [Am] a [G] new mass
So we [F] break it up with the heat
[G] Could have had [F] a _ model
[G] _ Without a [Am] scalar _ field
[G] _ But symmetry [F] _ requires a new mass
So we [G] break it up with the heat
_ Grow _ your vacuum to minimal [Am] potential _
Break your [Bb] SU2 down to massless moles _
Into mass terms of gauge bosons they go
For [A] me I'm sinking like gears [G] into stars
[Am] _ _ _ _ [G] _ We could have had [F] a _ _ model
[G] We could have had [Am] a _ model
[G] _ _ _ _
[F] Model, model, model
[G] We could have [Am] had a _ model
[G] _ Without a scalar [F] field
_ _ _ _ [G] But symmetry [Am] _ requires a new [G] mass
So we [F] break it up with the _ [G] heat
Could have [Am] had a model
_ _ [G] _ Without a [F] scalar _ field
_ [G] But symmetry [Am] requires a new [G] mass
So we [F] break it up with the heat
[G] _ _
_ _ _ Acapella Science _
[A] There's a collider [B] under Geneva _
[G] Reaching new energies that we've never achieved [D] before
[A] Finally we [B] can see with this machine
[G] A brand new data peak at 125 GeV
[D] See [E] how gluons [B] and vector bosons fuse _
[G] Muons and gamma rays emerge from something [D] new
[A] There's a [E] collider under [B] Geneva _
[G] Making one particle that we've never seen before
[F] A _ [G] complex scalar elusive [Em] boson
Escaped [F] detection by the _ lepantevatron
The [G] complex scalar, what [Em] is its purpose?
It's got me [E] thinking
We could have had [Am] a model
_ _ [G] _ Without a scalar [F] _ _ field
But [G] symmetry [A] requires [Am] a new [G] mass
So we [F] break it up with the heat
[G] _ _
[A] Baby, I have [E] a theory to be told
[G] A standard model used to discover our quantum world _
[A] _ _ _ [E] SU3U1 SU2's our gauge
[G] Make gauge transform and the equations should have changed
[F] _ The particle [G] goes and must all [Em] be massless
Because mass [F] terms vary under gauge transformation
The one [G] solution is [Em] spontaneous
See a symmetry break [F] it
We could have had [Am] a model
_ _ [G] _ Without a scalar [F] field
_ _ _ _ [G] But symmetry [A] requires [Am] a [G] new mass
So we [F] break it up with the heat
[G] Could have had [F] a _ model
[G] _ Without a [Am] scalar _ field
[G] _ But symmetry [F] _ requires a new mass
So we [G] break it up with the heat
_ Grow _ your vacuum to minimal [Am] potential _
Break your [Bb] SU2 down to massless moles _
Into mass terms of gauge bosons they go
For [A] me I'm sinking like gears [G] into stars
[Am] _ _ _ _ [G] _ We could have had [F] a _ _ model
[G] We could have had [Am] a _ model
[G] _ _ _ _
[F] Model, model, model
[G] We could have [Am] had a _ model
[G] _ Without a scalar [F] field
_ _ _ _ [G] But symmetry [Am] _ requires a new [G] mass
So we [F] break it up with the _ [G] heat
Could have [Am] had a model
_ _ [G] _ Without a [F] scalar _ field
_ [G] But symmetry [Am] requires a new [G] mass
So we [F] break it up with the heat
[G] _ _
_ _ _ Acapella Science _