“…This transition only exists in unconventional superconductors, like Fe-, Mn-, and Cr-based, and heavy fermions. 1 − 5 However, the mechanism of superconductivity has long been discussed. Recently, antiferromagnetic fluctuation has been a common interpretation for the formation of Cooper pairs for Fe-based systems, thus inducing the emergence of superconducting states.…”
The connection between
magnetism and superconductivity has long
been discussed since the discovery of Fe-based superconductors. Here,
we report the discovery of a pressure-induced transition from a spin
to a superconducting state in novel MnN
2
based on ab initio
calculations. The superconducting state can be obtained in two ways:
the first is the pressure-induced transition from an AFM-
P
2
1
/
m
to an NM-
I
4/
mmm
phase at 30 GPa, while the other is the pressure-induced
transition from an FM-
I
4/
mmm
phase
to magnetic vanishing at 14 GPa, which leads to a structural transition
with the distortion of octahedrons to tetragonal pyramids. NM-
I
4/
mmm-
MnN
2
is superconductive
with
T
c
≈ 17.6 K at 0 GPa. In the
second way, electronic structure calculations indicate that the system
transforms from a high-spin state to a low-spin state due to increasing
crystal-field splitting, causing disappearance of magnetism; more
electron occupancy around the Fermi level drives the emergence of
superconductivity. Remarkably,
I
4/
mmm-
MnN
2
can achieve mutual spin-to-superconducting state
transformation by pressure. Moreover, the AFM-
P
2
1
/
m-
MnN
2
phase is extremely incompressible
with the hardness above 20 GPa. Our results provide a reasonable and
systematic interpretation for the connection between magnetism and
superconductivity and give clues for achieving spin-to-superconducting
switching materials with certain crystal features.
“…This transition only exists in unconventional superconductors, like Fe-, Mn-, and Cr-based, and heavy fermions. 1 − 5 However, the mechanism of superconductivity has long been discussed. Recently, antiferromagnetic fluctuation has been a common interpretation for the formation of Cooper pairs for Fe-based systems, thus inducing the emergence of superconducting states.…”
The connection between
magnetism and superconductivity has long
been discussed since the discovery of Fe-based superconductors. Here,
we report the discovery of a pressure-induced transition from a spin
to a superconducting state in novel MnN
2
based on ab initio
calculations. The superconducting state can be obtained in two ways:
the first is the pressure-induced transition from an AFM-
P
2
1
/
m
to an NM-
I
4/
mmm
phase at 30 GPa, while the other is the pressure-induced
transition from an FM-
I
4/
mmm
phase
to magnetic vanishing at 14 GPa, which leads to a structural transition
with the distortion of octahedrons to tetragonal pyramids. NM-
I
4/
mmm-
MnN
2
is superconductive
with
T
c
≈ 17.6 K at 0 GPa. In the
second way, electronic structure calculations indicate that the system
transforms from a high-spin state to a low-spin state due to increasing
crystal-field splitting, causing disappearance of magnetism; more
electron occupancy around the Fermi level drives the emergence of
superconductivity. Remarkably,
I
4/
mmm-
MnN
2
can achieve mutual spin-to-superconducting state
transformation by pressure. Moreover, the AFM-
P
2
1
/
m-
MnN
2
phase is extremely incompressible
with the hardness above 20 GPa. Our results provide a reasonable and
systematic interpretation for the connection between magnetism and
superconductivity and give clues for achieving spin-to-superconducting
switching materials with certain crystal features.
“…The new class of ferromagnetic superconductors based on EuFe 2 As 2 parent compound is a unique playground in material science and solid state physics [1][2][3][4][5][6][7][8][9][10][11][12] due to accessible temperatures for the coexistence of superconducting and ferromagnetic orders on atomic scales of crystal lattice. Superconductivity in EuFe 2 As 2 -based ferromagnetic superconductors emerges by doping with phosphorus, [1][2][3][4] or rubidium.…”
In this work, fabrication and characterization of magnetic properties of EuFe 2 As 2 and EuRbFe 4 As 4 single crystals is reported. Magnetization measurements of samples with well defined thin film geometry and crystal orientation demonstrate a striking similarity in ferromagnetic properties of Eu subsystems in these two compounds. Measurements with magnetic field applied along ab crystal planes reveal meta-magnetic transition in both compounds. Numerical studies employing the J z1 and J z2 Heisenberg model suggest that the ground state of the magnetic order in Eu subsystem for both compounds is the helical spin order with the helical angle about 2π/5, while the meta-magnetic transition is the helix-to-fan first order phase transition.
“…The lateral geometry of LJJ makes them suitable for studying Josephson phenomena at the nanoscale by Scanning Probe Microscopies (SPM) such as Tunneling Microscopy and Spectroscopy [12,[19][20][21][22][23][24], Scanning SQUID [25][26][27][28][29] or Magnetic Force Microscopy (MFM) [13,[30][31][32]. The latter technique is particularly promising owing to its simplicity and its capacity to reveal the spatial distribution of the magnetic field over LJJ.…”
Lateral Josephson junctions (LJJ) made of two superconducting Nb electrodes coupled by Cufilm are applied to quantify the stray magnetic field of Co-coated cantilevers used in Magnetic Force Microscopy (MFM). The interaction of the magnetic cantilever with LJJ is reflected in the electronic response of LJJ as well as in the phase shift of cantilever oscillations, simultaneously measured. The phenomenon is theorized and used to establish the spatial map of the stray field. Based on our findings, we suggest integrating LJJs directly on the tips of cantilevers and using them as nanosensors of local magnetic fields in Scanning Probe Microscopes. Such probes are less invasive than conventional magnetic MFM cantilevers and simpler to realize than SQUID-on-tip sensors. [1].
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