Molecule-based magnets

Last updated

Molecule-based magnets (MBMs) or molecular magnets are a class of materials capable of displaying ferromagnetism and other more complex magnetic phenomena. This class expands the materials properties typically associated with magnets to include low density, transparency, electrical insulation, and low-temperature fabrication, as well as combine magnetic ordering with other properties such as photoresponsiveness. Essentially all of the common magnetic phenomena associated with conventional transition-metal magnets and rare-earth magnets can be found in molecule-based magnets. [1] [2] Prior to 2011, MBMs were seen to exhibit "magnetic ordering with Curie temperature (Tc) exceeding room temperature". [2] [3]

Contents

History

The first synthesis and characterization of MBMs was accomplished by Wickman and co-workers in 1967. This was a diethyldithiocarbamate-Fe(III) chloride compound. [4] [5]

In February 1992, Gatteschi and Sessoli published on MBMs with particular attention to the fabrication of systems in which stable organic radicals are coupled to metal ions. [6] At that date, the highest Tc on record was measured by SQUID magnetometer as 30K. [7]

The field exploded in 1996 with the publication of the book "Molecular Magnetism: From Molecular Assemblies to the Devices". [8]

In February 2007, de Jong et al. grew thin-film TCNE MBM in situ, [9] while in September 2007, photoinduced magnetism was demonstrated in a TCNE organic-based magnetic semiconductor. [10]

The June 2011 issue of Chemical Society Reviews was devoted to MBMs. In the editorial, written by Miller and Gatteschi, are mentioned TCNE and above-room-temperature magnetic ordering along with many other unusual properties of MBMs. [2]

Theory

The mechanism by which molecule-based magnets stabilize and display a net magnetic moment is different than that present in traditional metal- and ceramic-based magnets. For metallic magnets, the unpaired electrons align through quantum mechanical effects (termed exchange) by virtue of the way in which the electrons fill the orbitals of the conductive band. For most oxide-based ceramic magnets, the unpaired electrons on the metal centers align via the intervening diamagnetic bridging oxide (termed superexchange). The magnetic moment in molecule-based magnets is typically stabilized by one or more of three main mechanisms:[ citation needed ]

In general, molecule-based magnets tend to be of low dimensionality. Classic magnetic alloys based on iron and other ferromagnetic materials feature metallic bonding, with all atoms essentially bonded to all nearest neighbors in the crystal lattice. Thus, critical temperatures at which point these classical magnets cross over to the ordered magnetic state tend to be high, since interactions between spin centers is strong. Molecule-based magnets, however, have spin bearing units on molecular entities, often with highly directional bonding. In some cases, chemical bonding is restricted to one dimension (chains). Thus, interactions between spin centers are also limited to one dimension, and ordering temperatures are much lower than metal/alloy-type magnets. Also, large parts of the magnetic material are essentially diamagnetic, and contribute nothing to the net magnetic moment.[ citation needed ]

Applications

In 2015 oxo-dimeric Fe(salen)-based magnets ("anticancer nanomagnets") in a water suspension were shown to demonstrate intrinsic room temperature ferromagnetic behavior, as well as antitumor activity, with possible medical applications in chemotherapy, [11] [12] [13] [14] magnetic drug delivery, magnetic resonance imaging (MRI), and magnetic field-induced local hyperthermia therapy.

Background

Molecule-based magnets comprise a class of materials which differ from conventional magnets in one of several ways. Most traditional magnetic materials are comprised purely of metals (Fe, Co, Ni) or metal oxides (CrO2) in which the unpaired electrons spins that contribute to the net magnetic moment reside only on metal atoms in d- or f-type orbitals.[ citation needed ]

In molecule-based magnets, the structural building blocks are molecular in nature. These building blocks are either purely organic molecules, coordination compounds or a combination of both. In this case, the unpaired electrons may reside in d or f orbitals on isolated metal atoms, but may also reside in highly localized s and p orbitals as well on the purely organic species. Like conventional magnets, they may be classified as hard or soft, depending on the magnitude of the coercive field.[ citation needed ]

Another distinguishing feature is that molecule-based magnets are prepared via low-temperature solution-based techniques, versus high-temperature metallurgical processing or electroplating (in the case of magnetic thin films). This enables a chemical tailoring of the molecular building blocks to tune the magnetic properties.[ citation needed ]

Specific materials include purely organic magnets made of organic radicals for example p-nitrophenyl nitronyl nitroxides, [15] decamethylferrocenium tetracyanoethenide, [16] mixed coordination compounds with bridging organic radicals, [17] Prussian blue related compounds, [18] and charge-transfer complexes. [19]

Molecule-based magnets derive their net moment from the cooperative effect of the spin-bearing molecular entities, and can display bulk ferromagnetic and ferrimagnetic behavior with a true critical temperature. In this regard, they are contrasted with single-molecule magnets, which are essentially superparamagnets (displaying a blocking temperature versus a true critical temperature). This critical temperature represents the point at which the materials switches from a simple paramagnet to a bulk magnet, and can be detected by ac susceptibility and specific heat measurements.[ citation needed ]

Related Research Articles

<span class="mw-page-title-main">Diamagnetism</span> Magnetic property of ordinary materials

Diamagnetism is the property of materials that are repelled by a magnetic field; an applied magnetic field creates an induced magnetic field in them in the opposite direction, causing a repulsive force. In contrast, paramagnetic and ferromagnetic materials are attracted by a magnetic field. Diamagnetism is a quantum mechanical effect that occurs in all materials; when it is the only contribution to the magnetism, the material is called diamagnetic. In paramagnetic and ferromagnetic substances, the weak diamagnetic force is overcome by the attractive force of magnetic dipoles in the material. The magnetic permeability of diamagnetic materials is less than the permeability of vacuum, μ0. In most materials, diamagnetism is a weak effect which can be detected only by sensitive laboratory instruments, but a superconductor acts as a strong diamagnet because it entirely expels any magnetic field from its interior.

<span class="mw-page-title-main">Ferromagnetism</span> Mechanism by which materials form into and are attracted to magnets

Ferromagnetism is a property of certain materials that results in a significant, observable magnetic permeability, and in many cases, a significant magnetic coercivity, allowing the material to form a permanent magnet. Ferromagnetic materials are noticeably attracted to a magnet, a consequence of their substantial magnetic permeability.

<span class="mw-page-title-main">Magnetism</span> Class of physical phenomena

Magnetism is the class of physical attributes that occur through a magnetic field, which allows objects to attract or repel each other. Because both electric currents and magnetic moments of elementary particles give rise to a magnetic field, magnetism is one of two aspects of electromagnetism.

<span class="mw-page-title-main">Paramagnetism</span> Weak, attractive magnetism possessed by most elements and some compounds

Paramagnetism is a form of magnetism whereby some materials are weakly attracted by an externally applied magnetic field, and form internal, induced magnetic fields in the direction of the applied magnetic field. In contrast with this behavior, diamagnetic materials are repelled by magnetic fields and form induced magnetic fields in the direction opposite to that of the applied magnetic field. Paramagnetic materials include most chemical elements and some compounds; they have a relative magnetic permeability slightly greater than 1 and hence are attracted to magnetic fields. The magnetic moment induced by the applied field is linear in the field strength and rather weak. It typically requires a sensitive analytical balance to detect the effect and modern measurements on paramagnetic materials are often conducted with a SQUID magnetometer.

<span class="mw-page-title-main">Magnet</span> Object that has a magnetic field

A magnet is a material or object that produces a magnetic field. This magnetic field is invisible but is responsible for the most notable property of a magnet: a force that pulls on other ferromagnetic materials, such as iron, steel, nickel, cobalt, etc. and attracts or repels other magnets.

<span class="mw-page-title-main">Antiferromagnetism</span> Regular pattern of magnetic moment ordering

In materials that exhibit antiferromagnetism, the magnetic moments of atoms or molecules, usually related to the spins of electrons, align in a regular pattern with neighboring spins pointing in opposite directions. This is, like ferromagnetism and ferrimagnetism, a manifestation of ordered magnetism. The phenomenon of antiferromagnetism was first introduced by Lev Landau in 1933.

<span class="mw-page-title-main">Curie temperature</span> Temperature above which magnetic properties change

In physics and materials science, the Curie temperature (TC), or Curie point, is the temperature above which certain materials lose their permanent magnetic properties, which can (in most cases) be replaced by induced magnetism. The Curie temperature is named after Pierre Curie, who showed that magnetism was lost at a critical temperature.

<span class="mw-page-title-main">Ferrimagnetism</span> Type of magnetic phenomenon

A ferrimagnetic material is a material that has populations of atoms with opposing magnetic moments, as in antiferromagnetism, but these moments are unequal in magnitude, so a spontaneous magnetization remains. This can for example occur when the populations consist of different atoms or ions (such as Fe2+ and Fe3+).

A plastic magnet is a non-metallic magnet made from an organic polymer. One example is PANiCNQ, which is a combination of emeraldine-based polyaniline (PANi) and tetracyanoquinodimethane (TCNQ). When it was created by Pakistan born scientist Naveed A. Zaidi and colleagues at the University of Durham in 2004, it was the first magnetic polymer to function at room temperature.

A single-molecule magnet (SMM) is a metal-organic compound that has superparamagnetic behavior below a certain blocking temperature at the molecular scale. In this temperature range, an SMM exhibits magnetic hysteresis of purely molecular origin. In contrast to conventional bulk magnets and molecule-based magnets, collective long-range magnetic ordering of magnetic moments is not necessary.

<span class="mw-page-title-main">Magnetic structure</span> Ordered arrangement of magnetic spins in a material

The term magnetic structure of a material pertains to the ordered arrangement of magnetic spins, typically within an ordered crystallographic lattice. Its study is a branch of solid-state physics.

<span class="mw-page-title-main">Photomagnetism</span>

Photomagnetism is the effect in which a material acquires its ferromagnetic properties in response to light. The current model for this phenomenon is a light-induced electron transfer, accompanied by the reversal of the spin direction of an electron. This leads to an increase in spin concentration, causing the magnetic transition. Currently the effect is only observed to persist at very low temperature. But at temperatures such as 5K, the effect may persist for several days.

In magnetism, a nanomagnet is a nanoscopic scale system that presents spontaneous magnetic order (magnetization) at zero applied magnetic field (remanence).

<span class="mw-page-title-main">Iron oxide nanoparticle</span>

Iron oxide nanoparticles are iron oxide particles with diameters between about 1 and 100 nanometers. The two main forms are composed of magnetite and its oxidized form maghemite. They have attracted extensive interest due to their superparamagnetic properties and their potential applications in many fields including molecular imaging.

Magnetochemistry is concerned with the magnetic properties of chemical compounds. Magnetic properties arise from the spin and orbital angular momentum of the electrons contained in a compound. Compounds are diamagnetic when they contain no unpaired electrons. Molecular compounds that contain one or more unpaired electrons are paramagnetic. The magnitude of the paramagnetism is expressed as an effective magnetic moment, μeff. For first-row transition metals the magnitude of μeff is, to a first approximation, a simple function of the number of unpaired electrons, the spin-only formula. In general, spin–orbit coupling causes μeff to deviate from the spin-only formula. For the heavier transition metals, lanthanides and actinides, spin–orbit coupling cannot be ignored. Exchange interaction can occur in clusters and infinite lattices, resulting in ferromagnetism, antiferromagnetism or ferrimagnetism depending on the relative orientations of the individual spins.

Spin engineering describes the control and manipulation of quantum spin systems to develop devices and materials. This includes the use of the spin degrees of freedom as a probe for spin based phenomena. Because of the basic importance of quantum spin for physical and chemical processes, spin engineering is relevant for a wide range of scientific and technological applications. Current examples range from Bose–Einstein condensation to spin-based data storage and reading in state-of-the-art hard disk drives, as well as from powerful analytical tools like nuclear magnetic resonance spectroscopy and electron paramagnetic resonance spectroscopy to the development of magnetic molecules as qubits and magnetic nanoparticles. In addition, spin engineering exploits the functionality of spin to design materials with novel properties as well as to provide a better understanding and advanced applications of conventional material systems. Many chemical reactions are devised to create bulk materials or single molecules with well defined spin properties, such as a single-molecule magnet. The aim of this article is to provide an outline of fields of research and development where the focus is on the properties and applications of quantum spin.

<span class="mw-page-title-main">Hiizu Iwamura</span> Japanese chemist

Hiizu Iwamura is a Japanese chemist and Professor of Chemistry, Nihon University, as well as Professor Emeriti of the Institute for Molecular Science in Okazaki, the University of Tokyo, and Kyushu University in Japan.

Magnetic nanoparticle-based drug delivery is a means in which magnetic particles such as iron oxide nanoparticles are a component of a delivery vehicle for magnetic drug delivery, due to the simplicity with which the particles can be drawn to (external) magnetopuissant targets. Magnetic nanoparticles can impart imaging and controlled release capabilities to drug delivery materials such as micelles, liposomes, and polymers.

<span class="mw-page-title-main">Spinterface</span>

Spinterface is a term coined to indicate an interface between a ferromagnet and an organic semiconductor. This is a widely investigated topic in molecular spintronics, since the role of interfaces plays a huge part in the functioning of a device. In particular, spinterfaces are widely studied in the scientific community because of their hybrid organic/inorganic composition. In fact, the hybridization between the metal and the organic material can be controlled by acting on the molecules, which are more responsive to electrical and optical stimuli than metals. This gives rise to the possibility of efficiently tuning the magnetic properties of the interface at the atomic scale.

<span class="mw-page-title-main">Roberta Sessoli</span> Italian chemist

Roberta Sessoli is Professor of General and Inorganic Chemistry in the Department of Chemistry "Ugo Schiff" at the University of Florence. Renowned as a pioneer in the field of magnetic bistability and quantum effects in mesoscopic materials, her research centers around investigating the magnetic properties of molecular clusters and chains, with a focus on designing and characterizing molecular magnetic materials.

References

  1. [ dead link ] Molecule-Based Magnets Materials Research Society Retrieved on 20 December 2007
  2. 1 2 3 Miller, Joel S.; Gatteschi, Dante (2011). "Molecule-based magnets". Chemical Society Reviews. 40 (6): 3065–3066. doi:10.1039/C1CS90019F. PMID   21552607.
  3. Weber, Birgit; Jäger, Ernst-G. (2009). "Structure and Magnetic Properties of Iron(II/III) Complexes with N2O22-Coordinating Schiff Base Like Ligands (Eur. J. Inorg. Chem. 4/2009)". European Journal of Inorganic Chemistry. 2009 (4): 455. doi:10.1002/ejic.200990003.
  4. Wickman, H. H.; Trozzolo, A. M.; Williams, H. J.; Hull, G. W.; Merritt, F. R. (1967-03-10). "Spin-3/2 Iron Ferromagnet: Its Mössbauer and Magnetic Properties". Physical Review. American Physical Society (APS). 155 (2): 563–566. Bibcode:1967PhRv..155..563W. doi:10.1103/physrev.155.563. ISSN   0031-899X.
  5. Wickham, H. H.; Trozzolo, A. M.; Williams, H. J.; Hull, G. W.; Merritt, F. R. (1967-11-10). "Spin-3/2 Iron Ferromagnet: Its Mossbauer and Magnetic Properties". Physical Review. American Physical Society (APS). 163 (2): 526. Bibcode:1967PhRv..163..526W. doi: 10.1103/physrev.163.526 . ISSN   0031-899X.
  6. Gatteschi, Dante; Sessoli, Roberta (1992). "Molecular based magnetic materials". Journal of Magnetism and Magnetic Materials. 104–107: 2092–2095. Bibcode:1992JMMM..104.2092G. doi:10.1016/0304-8853(92)91683-K.
  7. Codjovi, Epiphane; Bergerat, Pierre; Nakatani, Keitaro; Pei, Yu; Kahn, Olivier (1992). "Molecular-based magnets studied with an ultrasensitive SQUID magnetometer". Journal of Magnetism and Magnetic Materials. 104–107: 2103–2104. Bibcode:1992JMMM..104.2103C. doi:10.1016/0304-8853(92)91687-O.
  8. Coronado, Eugenio; Delhaès, Pierre; Gatteschi, Dante; Miller, Joel S, eds. (1996). Molecular Magnetism: From Molecular Assemblies to the Devices. doi:10.1007/978-94-017-2319-0. ISBN   978-90-481-4724-3.
  9. De Jong, M. P.; Tengstedt, C.; Kanciurzewska, A.; Carlegrim, E.; Salaneck, W. R.; Fahlman, M. (2007). "Chemical bonding inV(TCNE)x(x~2)thin-film magnets grownin situ". Physical Review B. 75 (6): 064407. Bibcode:2007PhRvB..75f4407D. doi:10.1103/PhysRevB.75.064407.
  10. Yoo, Jung-Woo; Edelstein, R. Shima; Raju, N. P.; Lincoln, D. M.; Epstein, A. J. (2008). "Novel mechanism of photoinduced magnetism in organic-based magnetic semiconductor V(TCNE)x, x~2". Journal of Applied Physics. 103 (7): 07B912. Bibcode:2008JAP...103gB912Y. doi:10.1063/1.2830960.
  11. Eguchi, Haruki; Umemura, Masanari; Kurotani, Reiko; Fukumura, Hidenobu; Sato, Itaru; Kim, Jeong-Hwan; Hoshino, Yujiro; Lee, Jin; Amemiya, Naoyuki; Sato, Motohiko; Hirata, Kunio; Singh, David J.; Masuda, Takatsugu; Yamamoto, Masahiro; Urano, Tsutomu; Yoshida, Keiichiro; Tanigaki, Katsumi; Yamamoto, Masaki; Sato, Mamoru; Inoue, Seiichi; Aoki, Ichio; Ishikawa, Yoshihiro (2015). "A magnetic anti-cancer compound for magnet-guided delivery and magnetic resonance imaging". Scientific Reports. 5: 9194. Bibcode:2015NatSR...5E9194E. doi:10.1038/srep09194. PMC   4361848 . PMID   25779357.
  12. Sato, Itaru; Umemura, Masanari; Mitsudo, Kenji; Fukumura, Hidenobu; Kim, Jeong-Hwan; Hoshino, Yujiro; Nakashima, Hideyuki; Kioi, Mitomu; Nakakaji, Rina; Sato, Motohiko; Fujita, Takayuki; Yokoyama, Utako; Okumura, Satoshi; Oshiro, Hisashi; Eguchi, Haruki; Tohnai, Iwai; Ishikawa, Yoshihiro (2016). "Simultaneous hyperthermia-chemotherapy with controlled drug delivery using single-drug nanoparticles". Scientific Reports. 6: 24629. Bibcode:2016NatSR...624629S. doi:10.1038/srep24629. PMC   4840378 . PMID   27103308.
  13. Ohtake, Makoto; Umemura, Masanari; Sato, Itaru; Akimoto, Taisuke; Oda, Kayoko; Nagasako, Akane; Kim, Jeong-Hwan; Fujita, Takayuki; Yokoyama, Utako; Nakayama, Tomohiro; Hoshino, Yujiro; Ishiba, Mai; Tokura, Susumu; Hara, Masakazu; Muramoto, Tomoya; Yamada, Sotoshi; Masuda, Takatsugu; Aoki, Ichio; Takemura, Yasushi; Murata, Hidetoshi; Eguchi, Haruki; Kawahara, Nobutaka; Ishikawa, Yoshihiro (2017). "Hyperthermia and chemotherapy using Fe(Salen) nanoparticles might impact glioblastoma treatment". Scientific Reports. 7: 42783. Bibcode:2017NatSR...742783O. doi:10.1038/srep42783. PMC   5316938 . PMID   28218292.
  14. Kim, Jeong-Hwan; Eguchi, Haruki; Umemura, Masanari; Sato, Itaru; Yamada, Shigeki; Hoshino, Yujiro; Masuda, Takatsugu; Aoki, Ichio; Sakurai, Kazuo; Yamamoto, Masahiro; Ishikawa, Yoshihiro (2017). "Magnetic metal-complex-conducting copolymer core–shell nanoassemblies for a single-drug anticancer platform". NPG Asia Materials. 9 (3): e367. doi: 10.1038/am.2017.29 .
  15. Bulk ferromagnetism in the β-phase crystal of the p-nitrophenyl nitronyl nitroxide radical Chemical Physics Letters, Volume 186, Issues 4-5, 15 November 1991, Pages 401-404 Masafumi Tamura, Yasuhiro Nakazawa, Daisuke Shiomi, Kiyokazu Nozawa, Yuko Hosokoshi, Masayasu Ishikawa, Minuro Takahashi, Minoru Kinoshita doi : 10.1016/0009-2614(91)90198-I
  16. Chittipeddi, Sailesh; Cromack, K. R.; Miller, Joel S.; Epstein, A. J. (1987-06-22). "Ferromagnetism in molecular decamethylferrocenium tetracyanoethenide (DMeFc TCNE)". Physical Review Letters. American Physical Society (APS). 58 (25): 2695–2698. Bibcode:1987PhRvL..58.2695C. doi:10.1103/physrevlett.58.2695. ISSN   0031-9007. PMID   10034821.
  17. Caneschi, Andrea; Gatteschi, Dante; Sessoli, Roberta; Rey, Paul (1989). "Toward molecular magnets: the metal-radical approach". Accounts of Chemical Research. American Chemical Society (ACS). 22 (11): 392–398. doi:10.1021/ar00167a004. ISSN   0001-4842.
  18. Ferlay, S.; Mallah, T.; Ouahès, R.; Veillet, P.; Verdaguer, M. (1995). "A room-temperature organometallic magnet based on Prussian blue". Nature. Springer Nature. 378 (6558): 701–703. Bibcode:1995Natur.378..701F. doi:10.1038/378701a0. ISSN   0028-0836. S2CID   4261137.
  19. Miller, Joel S.; Epstein, Arthur J.; Reiff, William M. (1988). "Ferromagnetic molecular charge-transfer complexes". Chemical Reviews. American Chemical Society (ACS). 88 (1): 201–220. doi:10.1021/cr00083a010. ISSN   0009-2665.