Proton magnetic moment

The proton magnetic moment is the magnetic dipole moment of the proton, symbol μ_p. Protons and neutrons, both nucleons, comprise the nucleus of an atom, and both nucleons act as small magnets whose strength is measured by their magnetic moments. The magnitude of the proton's magnetic moment indicates that the proton is not an elementary particle.

Description

CODATA's recommended value for the magnetic moment of the proton is μ_p = 2.7928473508(85) μ_N.[1] A more precise measurement has since been claimed, with a result of μ_p = 2.79284734462(82) μ_N, for an 11-fold improvement in precision.[2] In these values, μ_N is the nuclear magneton, a physical constant and standard unit for the magnetic moments of nuclear components. In SI units, the CODATA value of μ_p is 1.4106067873(97)×10⁻²⁶ J⋅T⁻¹ (1.5210322053(46)×10⁻³ μ_B). A magnetic moment is a vector quantity, and the direction of the proton's magnetic moment is defined by its spin. The torque on the proton resulting from an external magnetic field is towards aligning the proton's spin vector in the same direction as the magnetic field vector.

The nuclear magneton is the spin magnetic moment of a Dirac particle, a charged, spin 1/2 elementary particle, with a proton's mass m_p. In SI units, the nuclear magneton is

${\displaystyle \mu _{\mathrm {N} }={{e\hbar } \over {2m_{\mathrm {p} }}}}$

where e is the elementary charge and ħ is the reduced Planck constant. The magnetic moment of this particle is parallel to its spin. Since the proton has charge +1 e, it should have magnetic moment equal to 1 μ_N by this expression. The larger magnetic moment of the proton indicates that it is not an elementary particle. The sign of the proton's magnetic moment is that of a positively charged particle. Similarly, the fact that the magnetic moment of the neutron, μ_n = −1.913 μ_N, is finite and negative indicates that it too is not an elementary particle.[3] Protons and neutrons are composed of quarks, and the magnetic moments of the quarks can be used to compute the magnetic moments of the nucleons.

The magnetic moment of the antiproton is the same magnitude, but is of opposite sign, as that of the proton.

Measurement

The anomalously large magnetic moment of the proton was discovered in 1933 by Otto Stern in Hamburg.[4][5] Stern won the Nobel Prize in 1943 for this discovery.[6]

By 1934 groups led by Stern, now in Pittsburgh, and I. I. Rabi in New York had independently measured the magnetic moments of the proton and deuteron.[7][8][9] While the measured values for these particles were only in rough agreement between the groups, the Rabi group confirmed the earlier Stern measurements that the magnetic moment for the proton was unexpectedly large.[10][11] Since a deuteron is composed of a proton and a neutron with aligned spins, the neutron's magnetic moment could be inferred by subtracting the deuteron and proton magnetic moments. The resulting value was not zero and had sign opposite to that of the proton. By the late 1930s accurate values for the magnetic moment of the proton had been measured by the Rabi group using newly developed nuclear magnetic resonance techniques.[11] The large value for the proton's magnetic moment and the inferred negative value for the neutron's magnetic moment were unexpected and raised many questions.[10] The anomalous values for the magnetic moments of the nucleons would remain a puzzle until the quark model was developed in the 1960s.

Proton g-factor and gyromagnetic ratio

The magnetic moment of a nucleon is sometimes expressed in terms of its g-factor, a dimensionless scalar. The conventional formula is

${\displaystyle {\boldsymbol {\mu }}={\frac {g\mu _{\mathrm {N} }}{\hbar }}{\boldsymbol {I}}}$

where μ is the intrinsic magnetic moment of the nucleon, I is the nuclear spin angular momentum, and g is the effective g-factor. For the proton, the magnitude of z component of I is 1/2 ħ, so the proton's g-factor, symbol g_p, is 5.585694713(46).[12]. By definition we take the z component in the above equation because when the field interacts with the nucleon, the change in energy is the dot product of magnetic field and magnetic moment.

The gyromagnetic ratio, symbol γ, of a particle or system is the ratio of its magnetic moment to its spin angular momentum, or

${\displaystyle {\boldsymbol {\mu }}=\gamma {\boldsymbol {I}}}$

For nucleons, the ratio is conventionally written in terms of the proton mass and charge, by the formula

${\displaystyle \gamma ={\frac {g\mu _{\mathrm {N} }}{\hbar }}=g{\frac {e}{2m_{p}}}}$

The proton's gyromagnetic ratio, symbol γ_p, is 2.675222005(63)×10⁸ rad⋅s⁻¹⋅T⁻¹.[13] The gyromagnetic ratio is also the ratio between the observed angular frequency of Larmor precession (in rad s⁻¹) and the strength of the magnetic field in proton NMR applications,[14] such as in MRI imaging or proton magnetometers. For this reason, the value of γ_p is often given in units of MHz/T. The quantity γ_p/2π ("gamma bar") is therefore convenient, which has the value 42.5774806(10) MHz⋅T⁻¹.[15]

Physical significance

When a proton is put into a magnetic field produced by an external source, it is subject to a torque tending to orient its magnetic moment parallel to the field (hence its spin also parallel to the field).[16] Like any magnet, the amount of this torque is proportional both to the magnetic moment and the external magnetic field. Since the proton has spin angular momentum, this torque will cause the proton to precess with a well-defined frequency, called the Larmor frequency. It is this phenomenon that enables the measurement of nuclear properties through nuclear magnetic resonance. The Larmor frequency can be determined by the product of the gyromagnetic ratio with the magnetic field strength. Since the sign of γ_p is positive, the proton's spin angular momentum precesses clockwise about the direction of the external magnetic field.

Since an atomic nucleus consists of a bound state of protons and neutrons, the magnetic moments of the nucleons contribute to the nuclear magnetic moment, or the magnetic moment for the nucleus as a whole. The nuclear magnetic moment also includes contributions from the orbital motion of the nucleons. The deuteron has the simplest example of a nuclear magnetic moment, with measured value 0.857 µ_N. This value is within 3% of the sum of the moments of the proton and neutron, which gives 0.879 µ_N. In this calculation, the spins of the nucleons are aligned, but their magnetic moments offset because of the neutron's negative magnetic moment.

Magnetic moment, quarks, and the Standard Model

Within the quark model for hadrons, such as the neutron, the proton is composed of one down quark (charge -1/3 e) and two up quarks (charge +2/3 e).[17] The magnetic moment of the proton can be modeled as a sum of the magnetic moments of the constituent quarks,[18] although this simple model belies the complexities of the Standard Model of particle physics.[19]

In one of the early successes of the Standard Model (SU(6) theory), in 1964 Mirza A. B. Beg, Benjamin W. Lee, and Abraham Pais theoretically calculated the ratio of proton to neutron magnetic moments to be −3/2, which agrees with the experimental value to within 3%.[20][21][22] The measured value for this ratio is −1.45989806(34).[23] A contradiction of the quantum mechanical basis of this calculation with the Pauli exclusion principle, led to the discovery of the color charge for quarks by Oscar W. Greenberg in 1964.[20]

From the nonrelativistic, quantum mechanical wavefunction for baryons composed of three quarks, a straightforward calculation gives fairly accurate estimates for the magnetic moments of protons, neutrons, and other baryons.[18] The calculation assumes that the quarks behave like pointlike Dirac particles, each having their own magnetic moment, as computed using an expression similar to the one above for the nuclear magneton. For a proton, the end result of this calculation is that the magnetic moment of the neutron is given by μ_p = 4/3 μ_u − 1/3 μ_d, where μ_u and μ_d are the magnetic moments for the up and down quarks, respectively. This result combines the intrinsic magnetic moments of the quarks with their orbital magnetic moments.

Baryon	Magnetic moment of quark model	Computed (${\displaystyle \mu _{\mathrm {N} }}$)	Observed (${\displaystyle \mu _{\mathrm {N} }}$)
p	4/3 μu − 1/3 μd	2.79	2.793
n	4/3 μd − 1/3 μu	−1.86	−1.913

While the results of this calculation are encouraging, the masses of the up or down quarks were assumed to be 1/3 the mass of a nucleon,[18] whereas the masses of these quarks are only about 1% that of a nucleon.[19] The discrepancy stems from the complexity of the Standard Model for nucleons, where most of their mass originates in the gluon fields and virtual particles that are essential aspects of the strong force.[19] Further, the complex system of quarks and gluons that constitute a neutron requires a relativistic treatment. A calculation of nucleon magnetic moments from first principles is not yet available.

See also

• Bohr magneton
• Electron magnetic moment
• Neutron magnetic moment
• Nuclear magnetic moment
• Anomalous magnetic moment
• Antiproton

References

1. Barry N. Taylor of the Data Center in close collaboration with Peter J. Mohr of the Physical Measurement Laboratory's Atomic Physics Division, Termed the "2014 CODATA recommended values," they are generally recognized worldwide for use in all fields of science and technology. The values became available on 25 June 2015 and replaced the 2010 CODATA set. They are based on all of the data available through 31 December 2014. Available: http://physics.nist.gov
2. Schneider, Georg; Mooser, Andreas; Bohman, Matthew; Schön, Natalie; Harrington, James; Higuchi, Takashi; Nagahama, Hiroki; Sellner, Stefan; Smorra, Christian; Blaum, Klaus; Matsuda, Yasuyuki; Quint, Wolfgang; Walz, Jochen; Ulmer, Stefan (2017). "Double-trap measurement of the proton magnetic moment at 0.3 parts per billion precision". Science. 358 (6366): 1081–1084. Bibcode:2017Sci...358.1081S. doi:10.1126/science.aan0207. PMID 29170238.
3. Bjorken, J.D.; Drell, S.D. (1964). Relativistic Quantum Mechanics. McGraw-Hill, New York. ISBN 978-0070054936.
4. Frisch, R.; Stern, O. (1933). "Über die magnetische Ablenkung von Wasserstoffmolekülen und das magnetische Moment des Protons. I / Magnetic Deviation of Hydrogen Molecules and the Magnetic Moment of the Proton. I". Z. Phys. 85 (1–2): 4–16. Bibcode:1933ZPhy...85....4F. doi:10.1007/bf01330773.
5. Esterman, I.; Stern, O. (1933). "Über die magnetische Ablenkung von Wasserstoffmolekülen und das magnetische Moment des Protons. II / Magnetic Deviation of Hydrogen Molecules and the Magnetic Moment of the Proton. I". Z. Phys. 85 (1–2): 17–24. Bibcode:1933ZPhy...85...17E. doi:10.1007/bf01330774.
6. "The Nobel Prize in Physics 1943". Nobel Foundation. Retrieved 2015-01-30.
7. Esterman, I.; Stern, O. (1934). "Magnetic moment of the deuton". Physical Review. 45 (10): 761(A109). Bibcode:1934PhRv...45..739S. doi:10.1103/PhysRev.45.739.
8. Rabi, I.I.; Kellogg, J.M.; Zacharias, J.R. (1934). "The magnetic moment of the proton". Physical Review. 46 (3): 157–163. Bibcode:1934PhRv...46..157R. doi:10.1103/physrev.46.157.
9. Rabi, I.I.; Kellogg, J.M.; Zacharias, J.R. (1934). "The magnetic moment of the deuton". Physical Review. 46 (3): 163–165. Bibcode:1934PhRv...46..163R. doi:10.1103/physrev.46.163.
10. Breit, G.; Rabi, I.I. (1934). "On the interpretation of present values of nuclear moments". Physical Review. 46 (3): 230–231. Bibcode:1934PhRv...46..230B. doi:10.1103/physrev.46.230.
11. John S. Rigden (2000). Rabi, Scientist and Citizen. Harvard University Press. ISBN 9780674004351.
12. "CODATA values of the fundamental constants". NIST.
13. "CODATA values of the fundamental constants". NIST.
14. Jacobsen, Neil E. (2007). NMR spectroscopy explained. Wiley-Interscience. ISBN 9780471730965.
15. "CODATA values of the fundamental constants". NIST.
16. B. D. Cullity; C. D. Graham (2008). Introduction to Magnetic Materials (2 ed.). Wiley-IEEE Press. p. 103. ISBN 978-0-471-47741-9.
17. Gell, Y.; Lichtenberg, D. B. (1969). "Quark model and the magnetic moments of proton and neutron". Il Nuovo Cimento A. Series 10. 61 (1): 27–40. Bibcode:1969NCimA..61...27G. doi:10.1007/BF02760010.
18. Perkins, Donald H. (1982), Introduction to High Energy Physics, Addison Wesley, Reading, Massachusetts, ISBN 978-0-201-05757-7
19. Cho, Adiran (2 April 2010). "Mass of the Common Quark Finally Nailed Down". http://news.sciencemag.org. American Association for the Advancement of Science. Retrieved 27 September 2014. External link in |website= (help)
20. Greenberg, O. W. (2009), "Color charge degree of freedom in particle physics", Compendium of Quantum Physics, Ed. D. Greenberger, K. Hentschel and F. Weinert, (Springer-Verlag, Berlin Heidelberg P: 109–111, arXiv:0805.0289, CiteSeerX 10.1.1.312.5798, doi:10.1007/978-3-540-70626-7_32, ISBN 978-3-540-70622-9
21. Beg, M.A.B.; Lee, B.W.; Pais, A. (1964). "SU(6) and electromagnetic interactions". Physical Review Letters. 13 (16): 514–517, erratum 650. Bibcode:1964PhRvL..13..514B. doi:10.1103/physrevlett.13.514.
22. Sakita, B. (1964). "Electromagnetic properties of baryons in the supermultiplet scheme of elementary particles". Physical Review Letters. 13 (21): 643–646. Bibcode:1964PhRvL..13..643S. doi:10.1103/physrevlett.13.643.
23. Mohr, P.J.; Taylor, B.N. and Newell, D.B. (2011), "The 2010 CODATA Recommended Values of the Fundamental Physical Constants" (Web Version 6.0). The database was developed by J. Baker, M. Douma, and S. Kotochigova. (2011-06-02). National Institute of Standards and Technology, Gaithersburg, Maryland 20899.

Bibliography

• Sergei Vonsovsky (1975). Magnetism of Elementary Particles. Mir Publishers.