41 research outputs found
Allmännyttans handlingsutrymme
Denna bok handlar om allmännyttans ställning på den svenska bostadsmarknaden. Den allmännyttiga hyresrätten har under efterkrigstiden varit en garant för en generell bostadspolitik med ambitionen om ”en bostad för alla”. Med de senaste årtiondenas marknadsinriktning av bostadsfrågorna har dock allmännyttans förutsättningar förändrats. En ny lag anger att allmännyttan både ska vara samhällsnyttig och verka utifrån affärsmässiga principer. Hur går detta ihop? Kommer allmännyttan att lyckas med denna dubbla uppgift? Boken belyser ur ett brett perspektiv de strategiska vägval som de nya förutsättningarna för med sig, inte bara för de kommunala bostadsföretagen utan också för svensk bostadspolitik framöver.
Boken är resultatet av ett flervetenskapligt forskningsprojekt som har engagerat ett dussintal forskare specialiserade på olika aspekter av allmännyttans förändrade roll. Forskningsledare och redaktör för boken har varit Tapio Salonen, professor i socialt arbete vid Malmö högskola
Marinite Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> (M = Co, Fe, Mn) and Li<sub>1</sub>Fe(SO<sub>4</sub>)<sub>2</sub>: Model Compounds for Super-Super-Exchange Magnetic Interactions
New
materials initially designed for battery electrodes are often of interest
for magnetic study, because their chemical compositions include 3d
transition metals. We report here on the magnetic properties of marinite
phases Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> (M = Fe, Co, Mn)
and Li<sub>1</sub>Fe(SO<sub>4</sub>)<sub>2</sub>, which all order
antiferromagnetically at low temperature. From neutron powder diffraction,
we propose a model for their ground-state magnetic structures. The
magnetism of marinite Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> compounds
unambiguously results from super-super-exchange interactions; therefore,
these materials can be considered as a model case for which the Goodenough–Kanamori–Anderson
rules can be tested
Magnetic Structures of Orthorhombic Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> (M = Co, Fe) and Li<sub><i>x</i></sub>Fe(SO<sub>4</sub>)<sub>2</sub> (<i>x</i> = 1, 1.5) Phases
We report herein
on the magnetic properties and structures of orthorhombic Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> (M = Co, Fe) and their oxidized phases
Li<sub><i>x</i></sub>Fe(SO<sub>4</sub>)<sub>2</sub> (<i>x</i> = 1, 1.5), which were previously studied as potential
cathode materials for Li-ion batteries. The particular structure of
these orthorhombic compounds (space group <i>Pbca</i>) consists
of a three-dimensional network of isolated MO<sub>6</sub> octahedra
enabling solely super-super-exchange interactions between transition
metals. We studied the magnetic properties of these phases via temperature-dependent
susceptibility measurements and applied neutron powder diffraction
experiments to solve their magnetic structures. All compounds present
an antiferromagnetic long-range ordering of the magnetic spins below
their Néel temperature. Their magnetic structures are collinear
and follow a spin sequence (+ + – – – –
+ +), with the time reversal associated with the inversion center,
a characteristic necessary for a linear magneto-electric effect. We
found that the orientation of the magnetic moments varies with the
nature of M. While Li<sub>2</sub>Co(SO<sub>4</sub>)<sub>2</sub> and
Li<sub>1</sub>Fe(SO<sub>4</sub>)<sub>2</sub> adopt the magnetic space
group <i>Pb</i>′<i>c</i>′<i>a</i>′, the magnetic space group for Li<sub>2</sub>Fe(SO<sub>4</sub>)<sub>2</sub> and Li<sub>1.5</sub>Fe(SO<sub>4</sub>)<sub>2</sub> is <i>P</i>112<sub>1</sub>′/<i>a</i>,
which might hint for a possible monoclinic distortion of their nuclear
structure. Moreover we compared the orthorhombic phases to their monoclinic
counterparts as well as to the isostructural orthorhombic Li<sub>2</sub>Ni(SO<sub>4</sub>)<sub>2</sub> compound. Finally, we show that this
possible magneto-electric feature is driven by the topology of the
magnetic interactions
Decoupling Cationic–Anionic Redox Processes in a Model Li-Rich Cathode via <i>Operando</i> X‑ray Absorption Spectroscopy
The
demonstration of reversible anionic redox in Li-rich layered
oxides has revitalized the search for higher energy battery cathodes.
To advance the fundamentals of this promising mechanism, we investigate
herein the cationic–anionic redox processes in Li<sub>2</sub>Ru<sub>0.75</sub>Sn<sub>0.25</sub>O<sub>3</sub>a model Li-rich
layered cathode in which Ru (cationic) and O (anionic) are the only
redox-active sites. We reveal its charge compensation mechanism and
local structural evolutions by applying <i>operando</i> (and
complementary <i>ex situ</i>) X-ray absorption spectroscopy
(XAS). Among other local effects, the anionic-oxidation-driven distortion
of the oxygen network around Ru atoms is thereby visualized. Oxidation
of lattice oxygen is also directly proven via hard X-ray photoelectron
spectroscopy (HAXPES). Furthermore, we demonstrate a spectroscopy-driven
visualization of electrochemical reaction paths, which enabled us
to neatly decouple the individual cationic–anionic <i>dQ</i>/<i>dV</i> contributions during cycling. We
hence establish the redox and structural origins of all <i>dQ</i>/<i>dV</i> features and demonstrate the vital role of anionic
redox in hysteresis and kinetics. These fundamental insights about
Li-rich systems are crucial for improving the existing anionic-redox-based
cathodes and evaluating the ones being discovered rapidly
Magnetic Structures of Orthorhombic Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> (M = Co, Fe) and Li<sub><i>x</i></sub>Fe(SO<sub>4</sub>)<sub>2</sub> (<i>x</i> = 1, 1.5) Phases
We report herein
on the magnetic properties and structures of orthorhombic Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> (M = Co, Fe) and their oxidized phases
Li<sub><i>x</i></sub>Fe(SO<sub>4</sub>)<sub>2</sub> (<i>x</i> = 1, 1.5), which were previously studied as potential
cathode materials for Li-ion batteries. The particular structure of
these orthorhombic compounds (space group <i>Pbca</i>) consists
of a three-dimensional network of isolated MO<sub>6</sub> octahedra
enabling solely super-super-exchange interactions between transition
metals. We studied the magnetic properties of these phases via temperature-dependent
susceptibility measurements and applied neutron powder diffraction
experiments to solve their magnetic structures. All compounds present
an antiferromagnetic long-range ordering of the magnetic spins below
their Néel temperature. Their magnetic structures are collinear
and follow a spin sequence (+ + – – – –
+ +), with the time reversal associated with the inversion center,
a characteristic necessary for a linear magneto-electric effect. We
found that the orientation of the magnetic moments varies with the
nature of M. While Li<sub>2</sub>Co(SO<sub>4</sub>)<sub>2</sub> and
Li<sub>1</sub>Fe(SO<sub>4</sub>)<sub>2</sub> adopt the magnetic space
group <i>Pb</i>′<i>c</i>′<i>a</i>′, the magnetic space group for Li<sub>2</sub>Fe(SO<sub>4</sub>)<sub>2</sub> and Li<sub>1.5</sub>Fe(SO<sub>4</sub>)<sub>2</sub> is <i>P</i>112<sub>1</sub>′/<i>a</i>,
which might hint for a possible monoclinic distortion of their nuclear
structure. Moreover we compared the orthorhombic phases to their monoclinic
counterparts as well as to the isostructural orthorhombic Li<sub>2</sub>Ni(SO<sub>4</sub>)<sub>2</sub> compound. Finally, we show that this
possible magneto-electric feature is driven by the topology of the
magnetic interactions
Magnetic Structures of Orthorhombic Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> (M = Co, Fe) and Li<sub><i>x</i></sub>Fe(SO<sub>4</sub>)<sub>2</sub> (<i>x</i> = 1, 1.5) Phases
We report herein
on the magnetic properties and structures of orthorhombic Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> (M = Co, Fe) and their oxidized phases
Li<sub><i>x</i></sub>Fe(SO<sub>4</sub>)<sub>2</sub> (<i>x</i> = 1, 1.5), which were previously studied as potential
cathode materials for Li-ion batteries. The particular structure of
these orthorhombic compounds (space group <i>Pbca</i>) consists
of a three-dimensional network of isolated MO<sub>6</sub> octahedra
enabling solely super-super-exchange interactions between transition
metals. We studied the magnetic properties of these phases via temperature-dependent
susceptibility measurements and applied neutron powder diffraction
experiments to solve their magnetic structures. All compounds present
an antiferromagnetic long-range ordering of the magnetic spins below
their Néel temperature. Their magnetic structures are collinear
and follow a spin sequence (+ + – – – –
+ +), with the time reversal associated with the inversion center,
a characteristic necessary for a linear magneto-electric effect. We
found that the orientation of the magnetic moments varies with the
nature of M. While Li<sub>2</sub>Co(SO<sub>4</sub>)<sub>2</sub> and
Li<sub>1</sub>Fe(SO<sub>4</sub>)<sub>2</sub> adopt the magnetic space
group <i>Pb</i>′<i>c</i>′<i>a</i>′, the magnetic space group for Li<sub>2</sub>Fe(SO<sub>4</sub>)<sub>2</sub> and Li<sub>1.5</sub>Fe(SO<sub>4</sub>)<sub>2</sub> is <i>P</i>112<sub>1</sub>′/<i>a</i>,
which might hint for a possible monoclinic distortion of their nuclear
structure. Moreover we compared the orthorhombic phases to their monoclinic
counterparts as well as to the isostructural orthorhombic Li<sub>2</sub>Ni(SO<sub>4</sub>)<sub>2</sub> compound. Finally, we show that this
possible magneto-electric feature is driven by the topology of the
magnetic interactions
Electrostatic Interactions versus Second Order Jahn–Teller Distortion as the Source of Structural Diversity in Li<sub>3</sub>MO<sub>4</sub> Compounds (M = Ru, Nb, Sb and Ta)
With
the advent of layered rocksalt oxides showing anionic redox
activity toward Li, there has been an increased focus on designing
new rocksalt structures and, more particularly, compounds pertaining
to the Li<sub>3</sub>MO<sub>4</sub> family. The structural richness
of this family is nested in its ability to host many different cations,
leading to the formation of superstructure patterns whose predictability
is still limited. Thus, there is a need to understand the formation
of such superstructures, as cationic arrangements have a crucial effect
on their physical properties. Herein we propose a combined experimental
and theoretical approach to understand the interactions governing
cation ordering in binary systems of general composition given by
Li<sub>3</sub>M<sub><i>y</i></sub>M′<sub>1–<i>y</i></sub>O<sub>4</sub> (M and M′ being Ru, Nb, Sb,
and Ta). Through complementary X-ray diffraction and X-ray absorption
spectroscopy techniques, we reveal a solid-solution behavior for the
Li<sub>3</sub>Ru<sub><i>y</i></sub>Sb<sub>1–<i>y</i></sub>O<sub>4</sub> system, as opposed to Li<sub>3</sub>Sb<sub><i>y</i></sub>Nb<sub>1–<i>y</i></sub>O<sub>4</sub> that enlists four rocksalt structures with different
cation orderings. We use DFT calculations to rationalize such a structural
diversity and find that it is controlled by a delicate balance between
electrostatic interactions and charge transfer due to a second order
Jahn–Teller distortion. This insight provides a new viewpoint
for understanding cationic arrangements in rocksalt structures and
guidelines to design novel phases for applications such as Li-ion
batteries or ionic conductors
Electrochemical Reduction of CO<sub>2</sub> Mediated by Quinone Derivatives: Implication for Li–CO<sub>2</sub> Battery
The
pivotal role of CO<sub>2</sub> played in global temperature
cycles has motivated the ongoing research on carbon capture and storage
(CCS). Within this context, Li–CO<sub>2</sub> battery, alike
the configuration of Li–O<sub>2</sub> battery, has been proposed
as a novel energy storage device with the potential to reduce CO<sub>2</sub>. Nevertheless, the highly negative potential required for
the electrochemical reduction of CO<sub>2</sub> adds difficulty to
the achievement of energy efficient Li–CO<sub>2</sub> battery.
Facilitating the electron transfer to this inert molecule, which largely
dictates the discharge voltage and rate capability of a Li–CO<sub>2</sub> battery, is therefore necessary. Herein, three types of quinones
have been surveyed, aiming to mediate the reduction of CO<sub>2</sub>, which is expected to result in lower overpotential than with a
direct electron transfer. We demonstrate by cyclic voltammetry that,
in the presence of quinones, CO<sub>2</sub> reduction proceeds through
an intermolecular interaction between CO<sub>2</sub> and quinone dianion.
Importantly, such catalytic CO<sub>2</sub> reduction reaction is associated
with the molecular structure of quinones, the supporting cation (e.g.,
Li<sup>+</sup>), and the electrolyte solvent. Furthermore, Li–CO<sub>2</sub> battery mediated by 2,5-di<i>tert</i>-butyl-1,4-benzoquinone
with Li<sub>2</sub>CO<sub>3</sub> as the ultimate discharge product
is achieved. This study validates the concept of using quinones as
chemical catalysts to promote CO<sub>2</sub> reduction in Li–CO<sub>2</sub> battery. Besides, battery performance and NMR analysis together
suggest that side reactions involving quinone itself and other cell
components occur
Electrostatic Interactions versus Second Order Jahn–Teller Distortion as the Source of Structural Diversity in Li<sub>3</sub>MO<sub>4</sub> Compounds (M = Ru, Nb, Sb and Ta)
With
the advent of layered rocksalt oxides showing anionic redox
activity toward Li, there has been an increased focus on designing
new rocksalt structures and, more particularly, compounds pertaining
to the Li<sub>3</sub>MO<sub>4</sub> family. The structural richness
of this family is nested in its ability to host many different cations,
leading to the formation of superstructure patterns whose predictability
is still limited. Thus, there is a need to understand the formation
of such superstructures, as cationic arrangements have a crucial effect
on their physical properties. Herein we propose a combined experimental
and theoretical approach to understand the interactions governing
cation ordering in binary systems of general composition given by
Li<sub>3</sub>M<sub><i>y</i></sub>M′<sub>1–<i>y</i></sub>O<sub>4</sub> (M and M′ being Ru, Nb, Sb,
and Ta). Through complementary X-ray diffraction and X-ray absorption
spectroscopy techniques, we reveal a solid-solution behavior for the
Li<sub>3</sub>Ru<sub><i>y</i></sub>Sb<sub>1–<i>y</i></sub>O<sub>4</sub> system, as opposed to Li<sub>3</sub>Sb<sub><i>y</i></sub>Nb<sub>1–<i>y</i></sub>O<sub>4</sub> that enlists four rocksalt structures with different
cation orderings. We use DFT calculations to rationalize such a structural
diversity and find that it is controlled by a delicate balance between
electrostatic interactions and charge transfer due to a second order
Jahn–Teller distortion. This insight provides a new viewpoint
for understanding cationic arrangements in rocksalt structures and
guidelines to design novel phases for applications such as Li-ion
batteries or ionic conductors
Magnetic Structures of Orthorhombic Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> (M = Co, Fe) and Li<sub><i>x</i></sub>Fe(SO<sub>4</sub>)<sub>2</sub> (<i>x</i> = 1, 1.5) Phases
We report herein
on the magnetic properties and structures of orthorhombic Li<sub>2</sub>M(SO<sub>4</sub>)<sub>2</sub> (M = Co, Fe) and their oxidized phases
Li<sub><i>x</i></sub>Fe(SO<sub>4</sub>)<sub>2</sub> (<i>x</i> = 1, 1.5), which were previously studied as potential
cathode materials for Li-ion batteries. The particular structure of
these orthorhombic compounds (space group <i>Pbca</i>) consists
of a three-dimensional network of isolated MO<sub>6</sub> octahedra
enabling solely super-super-exchange interactions between transition
metals. We studied the magnetic properties of these phases via temperature-dependent
susceptibility measurements and applied neutron powder diffraction
experiments to solve their magnetic structures. All compounds present
an antiferromagnetic long-range ordering of the magnetic spins below
their Néel temperature. Their magnetic structures are collinear
and follow a spin sequence (+ + – – – –
+ +), with the time reversal associated with the inversion center,
a characteristic necessary for a linear magneto-electric effect. We
found that the orientation of the magnetic moments varies with the
nature of M. While Li<sub>2</sub>Co(SO<sub>4</sub>)<sub>2</sub> and
Li<sub>1</sub>Fe(SO<sub>4</sub>)<sub>2</sub> adopt the magnetic space
group <i>Pb</i>′<i>c</i>′<i>a</i>′, the magnetic space group for Li<sub>2</sub>Fe(SO<sub>4</sub>)<sub>2</sub> and Li<sub>1.5</sub>Fe(SO<sub>4</sub>)<sub>2</sub> is <i>P</i>112<sub>1</sub>′/<i>a</i>,
which might hint for a possible monoclinic distortion of their nuclear
structure. Moreover we compared the orthorhombic phases to their monoclinic
counterparts as well as to the isostructural orthorhombic Li<sub>2</sub>Ni(SO<sub>4</sub>)<sub>2</sub> compound. Finally, we show that this
possible magneto-electric feature is driven by the topology of the
magnetic interactions