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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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Axions 527<br />

or axion decay constant. Axions must be fundamentally m<strong>as</strong>sless so that<br />

all observable effects remain unchanged under a global shift a(x) →<br />

a(x) + a 0 where a 0 is a constant. (A m<strong>as</strong>s term 1 2 m2 aa 2 would spoil this<br />

possibility.) This invariance allows one to absorb Θ in the definition of<br />

the axion field. Including a kinetic term, Eq. (14.1) is replaced by<br />

L Θ → L a = 1 2 (∂ µa) 2 −<br />

α s<br />

8π f a<br />

a G ˜G . (14.3)<br />

It conserves CP because axions were <strong>as</strong>sumed to be pseudoscalar (odd<br />

under CP), similar to neutral pions.<br />

Even though axions were constructed to be m<strong>as</strong>sless they acquire an<br />

effective m<strong>as</strong>s by their interaction with gluons. It induces transitions to<br />

qq states and thus to neutral pions (Fig. 14.1) which means physically<br />

that a and π ◦ mix with each other. Axions thereby pick up a small m<strong>as</strong>s<br />

which is approximately given by (Bardeen and Tye 1978; Kand<strong>as</strong>wamy,<br />

Salomonson, and Schechter 1978)<br />

m a f a ≈ m π f π , (14.4)<br />

where m π = 135 MeV is the pion m<strong>as</strong>s and f π ≈ 93 MeV its decay<br />

constant. This m<strong>as</strong>s term implies that at low energies the axion Lagrangian<br />

contains a potential V (a) which expands to lowest order <strong>as</strong><br />

1<br />

2 m2 aa 2 . Because of the invariance of L Θ with respect to Θ → Θ + 2π<br />

the gluon-induced potential V (a) is a function periodic with 2πf a .<br />

Fig. 14.1. Axion mixing with qq states and thus π ◦ . The curly lines represent<br />

gluons, the solid lines quarks.<br />

The ground state of the axion field is at the minimum of its potential<br />

at a = 0, explaining the absence of a neutron electric dipole<br />

moment. If one could produce a static nonvanishing axion field a 0 in<br />

some region of space, neutrons there would exhibit an electric dipole<br />

moment corresponding to Θ = −a 0 /f a .<br />

The Lagrangian Eq. (14.3) is the minimal ingredient <strong>for</strong> any axion<br />

model: the aG ˜G coupling is their defining feature <strong>as</strong> opposed to<br />

other pseudoscalar particles. Then axions inevitably acquire an effective<br />

m<strong>as</strong>s at low energies. Thus the concept of a “m<strong>as</strong>sless axion” <strong>for</strong><br />

some arbitrary pseudoscalar is a contradiction in terms.

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