Skip to main content  ∨   Page logos with links to institutions:
Max Planck Society Max Planck Institute for Nuclear Physics University of Heidelberg
Stored and Cooled Ions Division
Max Planck SocietyMax Planck Institute for Nuclear PhysicsUniversity of Heidelberg Stored and Cooled Ions Division
Superordinated navigation: MPIK Homepage  |  Home  |  Deutsch  |  Sitemap  |  Search  |  Contact
Section navigation:

Contact  Contact

Tel.: +49 6221 516-851
Fax: +49 6221 516-852
Postal Address
Max Planck Institute for Nuclear Physics
P.O. Box 10 39 80
69029 Heidelberg
Visitor Address
Max Planck Institute for Nuclear Physics
Saupfercheckweg 1
Building: Gentner lab,
room 134
69117 Heidelberg


Current News

24.11.17: Most precise measurement of the proton magnetic moment by an optimized double Penning-trap technique

The proton is one of the central building blocks of stable matter. For that reason the precise knowledge of its fundamental properties such as its mass (see our news of 18.07.17), lifetime, charge radius and magnetic moment is of great importance and thus the subject of many contemporary physics research programs. The mass, for example, is an input parameter for precise quantum electrodynamics calculations and the lower bound of the proton lifetime sets constraints on possible baryon number violation.
Apart from its fundamental nature, the proton is one of the few particles, which is comparable to its antiparticle – the antiproton. This allows for a test of the Charge, Parity, and Time Reversal (CPT) symmetry of the Standard Model of particle physics and Big Bang cosmology, which postulates that the fundamental properties of a particle and its antiparticle are exactly equal. Therefore, particles and antiparticles should have been created with same amounts. The lack of antimatter in our Universe, however, is in contradiction with this assumed matter-antimatter symmetry of the Standard Model. One possible explanation of the baryon asymmetry of the Universe is a violation of CPT invariance. Therefore, the measurement of minutest differences between the properties of a proton and its corresponding antiparticle, the antiproton, provides a precise test of the particle-antiparticle equality in the baryonic sector and of the CPT symmetry of the Standard Model.
The proton magnetic moment μp was directly measured in 2014 at the University of Mainz with a unprecedented fractional precision of 3.3 parts per billion (see our news of 28.05.14) using a novel double Penning-trap technique. Since then, the researchers at Mainz have developed techniques that enabled them to improve the measurement of the proton magnetic moment by more than one order of magnitude.

In a recent article published in "Science", G. Schneider et al. report on a direct high-precision measurement of the magnetic moment of the proton μp in units of the nuclear magneton μN. The measurement has been carried out in an improved double Penning-trap system at the University of Mainz, Germany.
A Penning trap is formed by a superposition of an electrostatic quadrupole potential and a homogeneous magnetic field B0, which was at 1.9 T in the described proton experiment.
The measurement of the frequency ratio νL/νc of the Larmor frequency and the cyclotron frequency allows the determination of the magnetic moment of a single proton in the Penning trap independent from the magnetic field B0. The cyclotron frequency νc can be determined from the three harmonic components νz, ν+, and ν- of the proton motion in the Penning trap using the invariance theorem: νc2 = ν+2 + νz2 + ν-2. The axial frequency νz of the stored proton is directly observed by non-destructive image current detection. The modified cyclotron frequency ν+ and the magnetron frequency ν- are measured by sideband coupling.
Since the Larmor frequency νL is not accompanied by an oscillating charge it cannot be determined by image current detection but by means of spin-transition spectroscopy. The superimposition of an inhomogeneous magnetic field, called a "magnetic bottle", couples the spin-magnetic moment of the proton to its axial oscillation frequency and thus allows to apply non-destructive detection of spin transitions (spin flips) using the continuous Stern-Gerlach effect.
However, the strong magnetic bottle broadens the Larmor resonance line significantly and limits the measurement to a relative precision of order 10-6 (p.p.m.). The application of a double Penning-trap technique overcomes this problem by using two separate Penning traps which are interconnected by a transport section. A precision trap (PT) with a nearly homogenous magnetic field is used for high-precision measurements of νc and νL and an analysis trap (AT) with the magnetic bottle is deployed for spin state detection of the proton. By applying this method, the proton g-factor measurement in 2014 at Mainz reached a relative precision of 3.3 p.p.b..

With respect to the proton measurements in 2014 the recent proton experiment at Mainz used an optimized double Penning-trap technique. The trap geometry was optimized to reach a higher magnetic homogeneity in the precision trap. Together with a superconducting self-shielding coil this allowed to improve the cyclotron stability by one order of magnitude. The width of the g-factor resonance, a major limitation in the previous measurement, was reduced by carefully optimizing the Larmor rf drive to probe the resonance. The particle preparation time for each individual measurement cycle could be reduced by applying a significantly improved superconducting detector for the modified cyclotron frequency ν+. This enabled a twice as high data acquisition rate which greatly increased statistics. Furthermore, the simultaneous measurement of νL and ν+ instead of a sequential determination ensured that νL and ν+ were measured at the same energies and times which eliminated many systematic shift contributions.
The final result of the determined proton magnetic moment in units of the nuclear magneton has a fractional precision of 0.3 p.p.b. (3·10-10): μp = 2.792 847 344 62(75)(34) μN. The first value in parentheses is the statistical uncertainty and the second one the systematic uncertainty. The new value of μp is in agreement with the currently accepted CODATA (Committee on Data for Science and Technology) value, but a factor of ten more precise. It improves the 3.3 p.p.b. precision of the μp measurement in 2014 at Mainz by a factor of eleven.

The BASE collaboration external Link recently measured the antiproton magnetic moment with a fractional precision of 1.5 p.p.b. (see our news of 18.10.17).
The recent results for the magnetic moments of the proton and the antiproton enable a test of the fundamental symmetry between matter and antimatter in the baryonic sector at the 10-9 - 10-10 level. The researchers expect that proton/antiproton magnetic moment measurements on the parts per trillion level (10-12) will become possible by reducing the particle preparation times by more than two orders of magnitude using sympathetically cooled protons/antiprotons by coupling them to laser cooled beryllium ions.

Please read more in the "Science" article ... >

A radio report external Link on the most precise measurement of the proton magnetic moment (start at 2:15 min.).

Further press releases:

07.11.17: Mass measurements on copper isotopes strengthen the prediction of a new island of inversion

In atomic nuclei the protons and neutrons occupy quantum levels that are separated by energy gaps. This leads to the ordering of the energy levels of the nucleons in the simple nuclear shell model. It successfully describes the nuclear structure near the valley of stability and explains the exceptional stability of nuclei with completely filled proton or neutron shells (i.e. magic proton or neutron numbers). However, over the years studies of exotic neutron-rich nuclei have shown that the postulated stability of nuclei with magic numbers can disappear. Today it is known that the shell-model magic numbers N = 8, 20, 28, and 40 are broken at the so called islands of inversion. Improved shell-model calculations predict a fifth island of inversion for Z < 28. Thus, the Z = 28, N = 50 region of the nuclear chart is a focus of today’s experimental and theoretical nuclear structure research. The doubly magic exotic nuclide 78Ni is of special interest and it is an open question, whether it retains the exceptional stability of the classic closed-shell nuclides. Furthermore, recent studies by laser spectroscopy offered strong evidence, that normal near-spherical and deformed structures coexist (so called shape coexistence) close to 78Ni. Copper isotopes in the vicinity of 78Ni provide an excellent proxy for probing the structure of 78Ni.

In a recently in Physical Review Letters published article A. Welker et al. report on high-precision mass measurements of the Z = 29 copper isotopes 75–79Cu (N = 46-50). The measurements were performed using the high-resolution multi-reflection time-of-flight mass spectrometer/separator (MR-TOF MS) ISOLTRAP external Link at CERN, Geneva.
A purified copper-ion ensemble was injected in a precision Penning trap, where the high-precision mass measurements were carried out by time-of-flight ion-cyclotron resonance (TOF-ICR). The TOF-ICR yields the atomic masses of the copper ions of interest by determination of the cyclotron-frequency ratio between the reference 85Rb+ ions and the copper ions. The use of the MR-TOF MS allowed measuring at a lower yield than would have been possible solely by Penning-trap mass spectrometry.
From the determined mass excesses the two-neutron separation energies S2n of the nuclides in the 78Ni region were deduced. The S2n values allow to probe the evolution of nuclear structure with neutron number. The S2n value is theoretically expected to drop between N = 50 and N = 52, which would be a well-known sign for magicity. Since the new masses do not extend beyond N = 50, it is not possible to observe the expected S2n drop. However, the new data differ significantly from that of previous results and the effect of the magic number is already noticeable in the S2n difference between N = 48 and N = 50. Thus, the high-precision mass measurements on 75–79Cu allow to define the mass surface above 78Ni and offer evidence for its doubly magic nature.

In addition to the mass experiments, large-scale shell-model calculations with the recently developed PFSDG-U interaction were performed. The new calculations predict shape coexistence in a doubly magic 78Ni and a new island of inversion for Z < 28. The calculated S2n values are in excellent agreement with the experimental results for Ni and Cu isotopes. This gives confidence in the underlying shell-model description of these exotic nuclides.

Please read more in the article ... >

The article has been selected for a Viewpoint in Physics. Please read also the viewpoint on the article external Link by Daniel Bazin.

Further information also in the press releases of the idw external Link and CERN external Link.

PRL Editor's Suggestion
The article has also been selected as "Editor's Suggestion". This is an award "based on the potential interest in the results presented and, importantly, on the success of the paper in communicating its message, in particular to readers from other fields" (see also here external Link)

18.10.17: Most precise measurement of the antiproton magnetic moment by a novel spectroscopy method

The Charge, Parity, and Time Reversal (CPT) symmetry of the Standard Model of particle physics implies the exact equality between the properties of a particle and its antiparticle. Thus, precise comparisons of the fundamental properties of matter/antimatter conjugates provide sensitive tests of CPT invariance. They provide data for Standard Model Extensions and contribute to a better understanding of the matter-antimatter imbalance of our universe.

Since the magnetic moment of the antiproton is 660 times smaller than the one of the positron, it is very difficult to measure its magnetic moment with high precision. Therefore, the antiproton magnetic moment is so far only known to a fractional uncertainty at the parts per million (p.p.m.) level (see our news of 18.01.17), whereas other matter/antimatter properties have been compared on the parts per billion (p.p.b.) level or better.
In 2014 the magnetic moment of the proton was measured directly at Mainz with 3.3 parts per billion (p.p.b.) precision (see our news of 28.05.14). These high-precision proton measurements were based on the application of the challenging double Penning-trap technique. The implementation of this method promised an improvement of the precision in antiproton magnetic moment measurements to the level of a few parts per billion.

In a recent article published in "Nature" C. Smorra and the BASE collaboration external Link reports on a measurement of the magnetic moment of the antiproton with a fractional precision of 1.5 p.p.b.. The measurement was performed at the Antiproton Decelerator (AD) external Link of CERN, Geneva, utilizing a novel two-particle spectroscopy method in an advanced cryogenic multi-Penning trap system.
The determination of the magnetic moment of a single particle in a Penning trap is based on the measurement of the frequency ratio of the Larmor frequency (νL) and the cyclotron frequency (νc). The measurement was mainly performed in two separate Penning traps, an analysis trap (AT) with an inhomogeneous magnetic field and a precision trap (PT) with a factor ~105 more homogeneous magnetic field B0 = 1.945 T.
In contrast to the double-Penning trap technique used in the measurement of the proton magnetic moment in 2014 at Mainz, the novel two-particle technique utilized a hot cyclotron antiproton for measurements of the cyclotron frequency νc, and a cold Larmor antiproton to determine the Larmor frequency νL. Thus, the new method eliminated the need of cyclotron cooling in each measurement cycle, and increased the sampling rate.

The Larmor frequency measurement is based on spin-transition spectroscopy. To this end, the spin-state of the antiproton is non-destructively determined in the magnetic bottle of the analysis trap, which couples the spin magnetic moment of the antiproton to its axial oscillation frequency νz. After the initial spin state is defined, the Larmor antiproton is moved into the precision trap where a spin transition for the spin-flip resonance is induced. The final state of the spin transition is analyzed by moving the Larmor antiproton back to the analysis trap.

The cyclotron antiproton is used to determine the magnetic field before and after each spin-flip attempt of the Larmor particle in the precision trap. It is moved to a park electrode before the Larmor antiproton is transported to the precision trap. The cyclotron frequency measurement is also based on image current detection. The three oscillation frequencies of the trapped antiproton are measured and the cyclotron frequency is obtained using the invariance theorem: νc2 = ν+2 + νz2 + ν-2.
The axial frequency νz of the stored antiprotons is directly observed by the image current detector. The modified cyclotron frequency ν+ and the magnetron frequency ν- were measured by coupling the axial and the radial modes using radio frequency drives on the motional sidebands at ν+ - νz resp. νz + ν-.

The novel two-particle spectroscopy method yielded a highly improved value for the magnetic moment of the antiproton in units of the nuclear magneton μN: μp = -2.792 847 344 1 (42) μN. This new value is about 350 times more precise than the result of the previous best μp measurement. It is consistent with the proton magnetic moment measured at Mainz in 2014, μp = 2.792 847 350 (9) μN, and is at the reached level of precision in agreement with CPT invariance.

The BASE collaboration expects that with a technically revised apparatus, including an improved magnetic shielding, an improved resistive cooling system for the cyclotron mode with lower temperature, and a precision trap with a 10-fold more homogeneous magnetic field, a ten-fold improved limit on CPT-odd interactions from proton/antiproton magnetic moment comparisons can be obtained in the future.

Please read more in the "Nature" article ... >

Further information also in the press release of the MPIK external Link.

Further press releases: