scholarly journals Intensity of the Earth's magnetic field: Evidence for a Mid-Paleozoic dipole low

2021 ◽  
Vol 118 (34) ◽  
pp. e2017342118
Author(s):  
Louise M. A. Hawkins ◽  
J. Michael Grappone ◽  
Courtney J. Sprain ◽  
Patipan Saengduean ◽  
Edward J. Sage ◽  
...  

The Mesozoic Dipole Low (MDL) is a period, covering at least ∼80 My, of low dipole moment that ended at the start of the Cretaceous Normal Superchron. Recent studies of Devonian age Siberian localities identified similarly low field values a few tens of million years prior to the Permo-Carboniferous Reverse Superchron (PCRS). To constrain the length and timing of this potential dipole low, this study presents paleointensity estimates from Strathmore (∼411 to 416 Ma) and Kinghorn (∼332 Ma) lava flows, United Kingdom. Both localities have been studied for paleomagnetic poles (Q values of 6 to 7), and the sites were assessed for their suitability for paleointensity from paleodirections, rock magnetic analysis, and microscopy. Thermal and microwave experiments were used to determine site mean paleointensity estimates of ∼3 to 51 μT (6 to 98 ZAm2) and 4 to 11 μT (9 to 27 ZAm2) from the Strathmore and Kinghorn localities, respectively. These, and all the sites from 200 to 500 Ma from the (updated) Paleointensity database (PINT15), were assessed using the Qualitative Paleointensity criteria (QPI). The procurement of reliable (QPI ≥ 5) weak paleointensity estimates from this and other studies indicates a period of low dipole moment (median field strength of 17 ZAm2) from 332 to 416 Ma. This “Mid-Paleozoic Dipole Low (MPDL)” bears a number of similarities to the MDL, including the substantial increase in field strength near the onset of the PCRS. The MPDL also adds support to the inverse relationship between reversal frequency and field strength and a possible ∼200-My cycle in paleomagnetic behavior relating to mantle convection.

2013 ◽  
Vol 20 (3) ◽  
pp. 327-336 ◽  
Author(s):  
Jaakko O. Nieminen ◽  
Jens Voigt ◽  
Stefan Hartwig ◽  
Hans Jürgen Scheer ◽  
Martin Burghoff ◽  
...  

Abstract The spin-lattice (T1) relaxation rates of materials depend on the strength of the external magnetic field in which the relaxation occurs. This T1 dispersion has been suggested to offer a means to discriminate between healthy and cancerous tissue by performing magnetic resonance imaging (MRI) at low magnetic fields. In prepolarized ultra-low-field (ULF) MRI, spin precession is detected in fields of the order of 10-100 μT. To increase the signal strength, the sample is first magnetized with a relatively strong polarizing field. Typically, the polarizing field is kept constant during the polarization period. However, in ULF MRI, the polarizing-field strength can be easily varied to produce a desired time course. This paper describes how a novel variation of the polarizing-field strength and duration can optimize the contrast between two types of tissue having different T1 relaxation dispersions. In addition, NMR experiments showing that the principle works in practice are presented. The described procedure may become a key component for a promising new approach of MRI at ultra-low fields


2003 ◽  
Vol 181 (5) ◽  
pp. 1211-1215 ◽  
Author(s):  
Thomas Magee ◽  
Marc Shapiro ◽  
David Williams

2007 ◽  
Vol 188 (4) ◽  
pp. 1094-1098 ◽  
Author(s):  
Timothy G. Sanders ◽  
Michael B. Zlatkin ◽  
Narayan Babu Paruchuri ◽  
Robert W. Higgins

2021 ◽  
Author(s):  
Sean Deoni ◽  
Muriel MK Bruchhage ◽  
Jennifer Beauchemin ◽  
Alexandra Volpe ◽  
Viren D'Sa ◽  
...  

Author(s):  
Yoshihiro Muragaki ◽  
Hiroshi Iseki ◽  
Takashi Maruyama ◽  
Masahiko Tanaka ◽  
Chie Shinohara ◽  
...  

Radiology ◽  
2019 ◽  
Vol 293 (2) ◽  
pp. 384-393 ◽  
Author(s):  
Adrienne E. Campbell-Washburn ◽  
Rajiv Ramasawmy ◽  
Matthew C. Restivo ◽  
Ipshita Bhattacharya ◽  
Burcu Basar ◽  
...  

Radiology ◽  
1991 ◽  
Vol 181 (1) ◽  
pp. 121-127 ◽  
Author(s):  
W W Orrison ◽  
G K Stimac ◽  
E A Stevens ◽  
D L LaMasters ◽  
M C Espinosa ◽  
...  

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