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Hydrogen Atom Spectrum and the Lamb Shift in Noncommutative QED

Hydrogen Atom Spectrum and the Lamb Shift in Noncommutative QED
Hydrogen Atom Spectrum and the Lamb Shift in Noncommutative QED

Hydrogen Atom Spectrum and the Lamb Shift in Noncommutative QED

M.Chaichian,1,*M.M.Sheikh-Jabbari,2,?and A.Tureanu1,?

1High Energy Physics Division,Department of Physics,University of Helsinki,Helsinki,Finland

and Helsinki Institute of Physics,P.O.Box64,FIN-00014Helsinki,Finland

2The Abdus Salam International Center for Theoretical Physics,Strada Costiera11,Trieste,Italy

(Received25October2000)

We have calculated the energy levels of the hydrogen atom as well as the Lamb shift within the

noncommutative quantum electrodynamics theory.The results show deviations from the usual QED both

on the classical and the quantum levels.On both levels,the deviations depend on the parameter of space/

space noncommutativity.

DOI:10.1103/PhysRevLett.86.2716PACS numbers:11.25.Sq,04.50.+h,12.20.Ds I.Introduction.—Recently,remotivated by string theory

arguments,noncommutative spaces(Moyal plane)have

been studied extensively.The noncommutative space can

be realized by the coordinate operators satisfying

??x m,?x n??i u mn,(1.1)

where?x are the coordinate operators and u mn is the non-

commutativity parameter and is of dimension of?length?2;

for a review on the string theory side,see[1].The

action for?eld theories on noncommutative spaces is then

obtained using the Weyl-Moyal correspondence[2–4],

according to which,in order to?nd the noncommutative

action,the usual product of?elds should be replaced by

the star product

?f?g??x??exp μi

2

u mn≠x

m

≠y

n

?

f?x?g?y?j x?y,(1.2)

where f and g are two arbitrary in?nitely differentiable

functions on R311.Performing explicit loop calculations,

for u0i?0cases(noncommutative space),it has been shown that noncommutative f4theory up to two loops

[3,5]and noncommutative QED up to one loop[4,6,7]are

renormalizable.For noncommutative space-time?u0i?

0?it has been shown that the theory is not unitary and

hence,as a?eld theory,it is not appealing[8].

Apart from the?eld theory interests which are more

academic,we are more interested in some possible

phenomenological consequences of noncommutativity in

space.Some of those results,all from the?eld theory

point of view,have been addressed in[4,9–11].How-

ever,perhaps a better starting point is to study quantum

mechanics(QM)on such noncommutative spaces.To

develop the noncommutative QM formulation we need to

introduce a Hamiltonian which governs the time evolution

of the system.We should also specify the phase space

and,of course,the Hilbert space on which these operators

act.As for the phase space,inferred from the string theory

[12,13],we choose

??x i,?x j??i u ij,

??x i,?p j??iˉh d ij,??p i,?p j??0.(1.3)

The Hilbert space can consistently be taken to be exactly

the same as the Hilbert space of the corresponding com-

mutative system.This assumption for the Hilbert space is

directly induced from the nonrelativistic limit of the related

noncommutative?eld theory,and one can really argue that

it satis?es all the needed properties of a physical Hilbert

space.The only nontrivial part of such a formulation is

to give the Hamiltonian.Once we have done it,the dy-

namical equation for the state j c?is the usual Schr?dinger

equation,i.e.,H j c??iˉh≠≠t j c?.

In this Letter we focus on the hydrogen atom and,using

the nonrelativistic limit of noncommutative QED results,

we propose the Hamiltonian describing the noncommuta-

tive hydrogen atom.Given the Hamiltonian and assum-

ing that the noncommutativity parameter?u ij?is small,we

study the spectrum of hydrogen atom.We show that be-

cause of noncommutativity,even at?eld theory tree level,

we have some corrections to the Lamb shift(2P1?2!

2S1?2transition).Since the noncommutativity in space

violates rotational symmetry,our Lamb shift corrections

have a preferred direction,and hence we call them“polar-

ized Lamb shift.”We also consider further corrections to

Lamb shift originating from the loop contributions in non-

commutative QED.In this way we will?nd some upper

bound for u.In addition,we study the Stark and Zeeman

effects for the noncommutative hydrogen atom.

II.Formulation of the noncommutative Hamiltonian.—

To start with,we propose the following Hamiltonian

for the noncommutative hydrogen atom.Of course,we

shall verify our proposal by a noncommutative QED

calculation:

H?

?p?p

2m

1V??x?,(2.1)

where the Coulomb potential in terms of the noncommu-

tative coordinates?x is

V?r??2

Ze2

p

?x?x

,(2.2)

with?p and?x satisfying(1.3).

Now,we note that there is a new coordinate system,

27160031-9007?01?86(13)?2716(4)$15.00?2001The American Physical Society

x i??x i1

1

2ˉh

u ij?p j,p i??p i,(2.3)

where the new variables satisfy the usual canonical com-mutation relations:

?x i,x j??0,

?x i,p j??iˉh d ij,

?p i,p j??0.(2.4) So,if in the Hamiltonian we change the variables?x i,?p i to x i,p i,the Coulomb potential becomes

V?r??2

Ze2

q

?x i2u ij p j?2ˉh??x i2u ik p k?2ˉh?

?2Ze 2

r 2Ze2

x i u ij p j

2ˉhr3

1O?u2?

?2Ze 2

r 2Ze2

?L??u

4ˉhr3

1O?u2?,(2.5)

where u i?e ijk u jk,?L??r3?p.

As??r3?p???u?2?r???u3?p?,it follows that the Coulomb potential can also be written as

V?r??2Ze2

r

2

e

4ˉh

??u3?p??

μ

2

Ze?r

r3

?

1O?u2?.

(2.6)

The other higher order terms,besides being higher powers in u,which in its own turn is very small,are also higher powers in momenta.

Our proposal for the Hamiltonian can be justi?ed from ?eld theory calculations.The electron-photon vertex func-tion at tree level in noncommutative QED is[4]

G m?e?i?2ˉh2?p3p0g m?e2?i?2ˉh2?p?q g m,(2.7) where p and p0are the incoming and outgoing electron momenta,respectively,q m is the photon momentum,p02 p?q,and

p3p0?p i u ij p0j,?q i?u ji q j. Expanding the exponential in powers of u and keeping only the?rst two terms,it appears that the second term will give rise to an electric dipole moment[14],which couples to an external electric?eld E as2??P???E where

?P i??21

2ˉh e?p i?

1

2ˉh

e u ij p j.(2.8)

This electric dipole moment,as we will see,changes the usual Lamb shift.Actually one can go further and prove that the potential(2.5),for all orders in u,is expected from the noncommutative QED starting from(2.7).This can be done noting that f?x i1e i??e e i?≠?≠x i?f?x?.

Our proposal for the noncommutative hydrogen atom Hamiltonian can be generalized to other systems,i.e.,tak-ing the usual Hamiltonian but now being a function of noncommutative coordinates[like(2.1)].However,our discussion based on noncommutative QED is applicable only when we deal with the“electromagnetic”interaction. In other words,at?eld theory tree level and in the non-relativistic limit,the noncommutativity of space is probed through the electric dipole moment of particles,whether fermions or bosons.

In our formulation for noncommutative quantum me-chanics,one can still use the usual de?nition for the proba-bility density,j c j2.However,one should be aware that there is no coordinate basis in this case.In our approach, since the noncommutativity parameter,if it is nonzero, should be very small compared to the length scales of the system,one can always treat the noncommutative effects as some perturbations of the commutative counterpart and hence,up to?rst order in u,we can use the usual wave functions and probabilities.

III.“Classical”spectrum for hydrogen atom in NC theory.—Using the usual perturbation theory,the leading corrections to the energy levels due to noncommutativity, i.e.,?rst order perturbation and in?eld theory tree level, are

D E H2atom

NC

?2?nl0jj0z j Ze

2

4ˉh

?L??u

r3

j nljj z?.(3.1) We note that the above expression is very similar to that of the spin-orbit coupling,where u l2

e

is now replacing the spin,?Sˉh,with l e being the electron Compton wave length. If we put u3?u and the rest of the u components to zero(which can be done by a rotation or a rede?nition of coordinates),then?L??u?L z u and,taking into account the fact that

?ljj z j L z j l0jj0z??j zˉh

μ

17

1

2l11

?

d ll0d j

z

j0z

,

j?l6

1

2

,

the energy level shift given by(3.1)becomes[15]

D E H2atom

NC

?2m e c

2

4

?Z a?4u

l2e

j z

μ

17

1

2l11

?

3f n,l d ll0d j

z

j0

z

(3.2) for j?l612and f n,l?1?n3l?l112??l11?.

It is worth noting that in order to?nd?1r3?,one should integrate over the wave functions from r?0;on the other hand,the approximation we are working in(dropping the terms higher order in u)is not valid for r&

p

u.However, since the wave function for l?0is zero at r?0,the result(3.2)still holds at this level.

The case of our interest,the2P1?2!2S1?2transition (Lamb shift),differs from the usual commutative case in which the shift depends only on the l quantum number and all the corrections are due to the?eld theory loop effects.The Lamb shift for the noncommutative hydrogen atom,besides the usual loop effects,depends on the j z

2717

quantum number (only for the 2P 1?2level,as the levels with l ?0are not affected)and is there,even in the ?eld theory tree level.Hence we call it polarized Lamb shift .More precisely,there is a new transition channel which is

opened because of noncommutativity:2P 21?21?2!2P 1?2

1?2,

with the notation nl j z

j for the energy levels.The usual Lamb shift,2P 1?2!2S 1?2,is now split into two parts,

2P 1?2

1?2!2S 1?2and 2P 21?21?2!2S 1?2,which means that the noncommutativity effects increase the widths and split the Lamb shift line by a factor proportional to u .

IV .One loop corrections.—In the usual commutative theory,the Lamb shift is believed to come from loop cor-rections to QED.In the usual case,both vertex corrections,in particular,the g 22factor in the spin-orbit coupling,and the corrections to photon propagator [16]are respon-sible for the Lamb shift.

A.Noncommutative one loop vertex corrections:Ac-cording to noncommutative QED one loop results,the elec-tric and magnetic dipole moments of the electron,as a Dirac particle,are [4]

??m ??2e 2mc μg ?S 1ag E 3p ˉh ?u l 2e ?,g ?21a p

,??P ??2e 4ˉh ??u 3?p ?μ113ag E p ?

.(4.1)Hence,the noncommutative one loop correction to the po-tential (2.5),originating from vertex corrections up to the

?rst order in u ,is

V 1Loop

NC vertex ?2Ze 24p g E a μ

3223??L ??u ˉhr 3.(4.2)

B.Noncommutative one loop photon propagator correc-tions:The photon propagator at one loop in the noncom-mutative QED,for small q ,?q is given by [6]P mn ?q ??e

2

16p 2?103

?g mn q 22q m q n ?3∑ln ?q 2?q 2?1

2

25q 2

m 2

∏132?q m ?q

n ?q 42

43q 2?q 2

?q m ?q n ?

,(4.3)where the term proportional to 2

25q 2

m 2is the fermionic loop contribution which,because of the cancellation in phase factors coming from noncommutativity,is the same as the usual QED result.From (4.3),by taking only the part of the propagator corresponding to timelike photons and reintroducing ˉh ,c factors,in the units where the Coulomb

potential is 2Ze 2

r ,we obtain

V 1Loop prop.?r ??2Ze 2a

103ˉh Z d 3q 12e 2i ?q ??r ?ˉ

h 3∑ln μ?q

2?q 2ˉh 4?

1225?q 2m 2

∏.(4.4)The second term in the integral yields the usual d 3?r ?-type

correction to the Coulomb potential.To work out the inte-gral in the ?rst term which is u dependent,let us assume that only u 12?u is nonzero.If we denote the integral by

I ?r ,u ?,then dI d u ?12p r u and thus I ?u ,r ??12p r ln ?uL 2

?,where L is a cutoff.This can be understood noting that,because of IR/UV mixing [4,6],the Fourier transformation

and also (4.3)are valid for 1

Lu &q &L .Putting all these results together,we have

V 1Loop prop.?r ?

?2

Ze 22p r 10a

3ln ?uL 2?2Ze 24a 15l 2e

d 3?r ?.(4.5)

The ?rst term,being proportional to 1

r ,can be under-stood as the normalization of charge at the one loop level [6];however,to ?nd the physical value of a (noncom-mutative QED coupling),one should study the Thomson limit of Compton scattering [17]for the noncommutative case [18].Summing up all the one loop contributions to the Lamb shift due to noncommutativity,(4.2)and (4.5),we get

D E 1Loop

NC

?2

1

2p m e c 2?Z a ?23∑5a 3ln ?uL 2?1n 22?Z a ?22u l 2e

3g E a μ322

3?j z ?171

2l 11?n 3l ?l 112

??l 11?∏.

(4.6)

One can use the data on the Lamb shift to impose some bounds on the value of the noncommutativity parameter,u .Of course,to do it,we need to consider only the classical (tree level)results,(3.2).Comparing these results,the contribution of (3.2)should be of the order of 10261027smaller than the usual one loop result,and hence

u l 2e

&1027

a or

u &?104GeV ?22.

This bound is indeed not a strong one,and one would need

some more precise experiments or data.Among other processes,the e 1e 2scattering data can provide a better bound on u [18].

V .Noncommutative Stark and Zeeman effects.—Stark effect:The potential energy of the atomic electron in an external electric ?eld oriented along the z axis is given,at tree level,by

V Stark ?eEz 1

e 4ˉ

h ??u 3?p ???E (5.1)

(neglecting the motion of the proton).

The change in the hydrogen atom energy level due to noncommutativity [the second term in (5.1)]is

D E NC Stark ??nl 0jj 0z j

e 4ˉ

h ??u 3?p

???E j nljj z ?.(5.2)

2718

Taking into account the fact that p i?m iˉh?x i,H0?,where H0is the unperturbed Hamiltonian,so that H0j nljj z??E n j nljj z?,the correction to the energy levels becomes

D E NC Stark~??u3?E?i?nl0jj0z j?x i,H0?j nljj z??0,(5.3)

meaning that,at tree level,the contribution to the Stark effect due to noncommutativity is zero.We also note that, adding the one loop corrections to electric dipole moment (4.1),the above result will not be changed.

Zeeman effect:The new parts which are added to the usual potential energy of the atom in a magnetic?eld,due to noncommutativity,are

V NC Zeeman?

e

2m e c

ag E m2e

3pˉh

μ

12f

m p

m e

?

?u??B,(5.4)

where f is a form factor of the order of unity,as the proton is not pointlike.As a result,the noncommutative contribu-tion to the Zeeman effect in the?rst order of perturbation theory is

D E NC Zeeman?

1

6p cˉh

e ag E m e

μ

12f

m p

m e

?

?u??B.(5.5)

VI.Conclusion.—We have presented the results on the classical Coulomb potential within the formulated non-commutative quantum mechanics for the hydrogen atom and have obtained the corrections to the Lamb shift using the noncommutative QED.If there exists any noncommu-tativity of space-time in nature,as it seems to emerge from different theories and arguments,its implications should appear in physical systems such as the one treated in this Letter.A detailed analysis of the results obtained here, together with the treatment of other fundamental and pre-cisely measured physical processes,will be given in a fur-ther communication[18].

We are grateful to A.Demichev,D.Demir,P.Preˇs najder, and especially to C.Montonen for many useful discus-sions and comments.This work was partially supported by the Academy of Finland,under Project No.163394.

A.T.thanks the World Laboratory,Lausanne,for?nancial support.The work of M.M.Sh.-J.was partly supported by the EC Contract No.ERBFMRX-CT

96-0090.

*Email address:Masud.Chaichian@helsinki.?

?Email address:jabbari@ictp.trieste.it

?On leave of absence from the Department of Theoretical Physics,“Al.I.Cuza”University of Iasi,Romania.

Email address:atureanu@pcu.helsinki.?

[1]N.Seiberg and E.Witten,J.High Energy Phys.09,032

(1999),and references therein.

[2]L.Alvarez-Gaume and S.R.Wadia,hep-th/0006219.

[3]A.Micu and M.M.Sheikh-Jabbari,hep-th/0008057.

[4]I.F.Riad and M.M.Sheikh-Jabbari,J.High Energy Phys.

0008,045(2000).

[5]I.Ya.Aref’eva,D.M.Belov,and A.S.Koshelev,Phys.

Lett.B476,431(2000).

[6]M.Hayakawa,hep-th/9912167.

[7]C.P.Martin and F.R.Ruiz,hep-th/0007131.

[8]J.Gomis and T.Mehen,Nucl.Phys.B591,265(2000);

M.Chaichian,A.Demichev,P.Preˇs najder,and A.Tureanu, hep-th/0007156.

[9]I.Mocioiu,M.Pospelov,and R.Roiban,Phys.Lett.B489,

390(2000).

[10]N.Chair and M.M.Sheikh-Jabbari,hep-th/0009037.

[11]M.M.Sheikh-Jabbari,Phys.Rev.Lett.84,5265(2000).

[12]F.Ardalan,H.Arfaei,and M.M.Sheikh-Jabbari,J.High

Energy Phys.9902,016(1999).

[13]P-M.Ho and S-C.Chu,Nucl.Phys.B550,151(1999).

[14]M.M.Sheikh-Jabbari,Phys.Lett.B455,129(1999).

[15]https://www.doczj.com/doc/ef5448283.html,ndau and E.M.Lifshitz,Quantum Mechanics:

Non-Relativistic Theory(Pergamon Press,New York, 1977).

[16]C.Itzykson and J-B.Zuber,Quantum Field Theory

(McGraw-Hill,New York,1980).

[17]H.D.Abarbanel and M.L.Goldberger,Phys.Rev.165,

1594(1968).

[18]Work in preparation.

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