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The Joy of Condensed Matter Physics
The Joy of Condensed Matter Physics
- Original source: https://www.forbes.com/sites/quora/2016/08/11/the-joy-of-condensed-matter-physics/
- Original author: Inna Vishik, then Assistant Professor of Physics at UC Davis
- Original publication: 2016-08-11, Forbes republication of a Quora answer
- Preservation copy: Stony Brook University PHY 555 course PDF, https://dreyer-research-group.github.io/Teaching/Phys555_Fall2022/Lecture1/Vishik-TheJoyOfCondensedMatterPhysics.pdf
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The Joy Of Condensed Matter Physics 8/15/22, 8:05 PM
The Joy Of Condensed Matter Physics
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Aug 11, 2016, 01:50pm EDT
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Why is condensed matter physics interesting? originally
appeared on Quora - the knowledge sharing network where
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The Joy Of Condensed Matter Physics 8/15/22, 8:05 PM
compelling questions are answered by people with unique
insights .
Answer by Inna Vishik, Assistant Professor of Physics at
I am drawn to condensed matter physics because it is
simultaneously useful and fundamental, simultaneously
mundane and fantastical, simultaneously large and small, and
most of all, some of the phenomena that are observed in
condensed matter systems are just flipping cool.
First, a definition of condensed matter. This field studies many
atom systems that are condensed (i.e. not a gas) but not too
condensed (i.e. not the inside of a neutron star). Condensed
matter physics in its broadest definition encompasses many
different subfields (cold atoms, biophysics, soft matter, solid
state physics, etc.). For this piece, I will focus on solid-state
physics (the study of crystalline solids; also called hard
condensed matter) with which I am most familiar.
With that disclaimer out of the way, back to our scheduled
programming …
Condensed matter physics is both useful and fundamental .
Many people who know a little bit about solid state physics know
that it gave us microscopic understanding of silicon and its native
oxide, which gave us solid-state transistors, which gave us every
computer and smartphone on the planet. But those same
semiconducting materials, when stacked on top of each other in a
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specific way, can produce a very pure 2-dimensional metal at the
interface. When this specially-prepared material is cooled down
to very low temperature (<4K, i.e. not useful) and subjected to a
large magnetic field (several Tesla, not useful), it exhibits
quantized conductance comprising the integer and fractional
quantum Hall effect, both of which garnered Nobel prizes in
physics. The former is used as a standard for electrical resistance
(useful after all), and the latter exhibits electron-like
quasiparticles that behave as if they have fractional charge
(whaa??).
On that note, condensed matter systems manifest other
quasiparticles (objects that behave like particles inside the solid
but don’t exist outside the solid) which are predicted in particle
physics but never observed in free space, such as majorana
fermions [1] and magnetic monopoles [2]. The quantum hall
effect is the intellectual predecessor to a subfield of solid-state
physics that is currently very trendy—topological materials,
including topological insulators, Dirac semimetals and Weyl
semimetals. These also connect to particle physics via
quasiparticles that behave like massless Dirac and Weyl fermions
(fundamental), and if they can be made superconducting in the
proper way, it is predicted that they will also manifest majorana
fermions which may be used for quantum computation [3]
(potentially useful).
Condensed matter physics is simultaneously mundane and
fantastical . I am typing this answer at my dining room table,
and I can use condensed matter physics to explain why various
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objects in my vicinity behave the way they do: why my ceramic
coffee mug is good for handling hot liquids and would break if I
dropped it, why my stainless steel fork does not attract a paper
clip right now but would if I held it up to a big honking magnet,
why my diamond is so flawless (when at a loss for a third item on
a list, quote Beyoncé).
These same materials can be implicated in my personal favorite
phenomenon in condensed matter physics—superconductivity—
in which a material suddenly loses its resistivity at low enough
temperature and can conduct a dissipationless current (basically,
a perpetual motion machine, if you can keep it cold enough).
Some of the highest temperature superconductors out there are
ceramic materials [4]. Iron (the main elemental constituent of
steel) can be compressed (but not nearly as much as a neutron
star) and become a superconductor [5]; or it can be alloyed with,
say, arsenic and barium to make a different type of high
temperature superconductor [6]. And diamond becomes
superconducting [7] if you dope it with an ample amount of
boron.
This juxtaposition between the mundane and the fantastical
also encompasses the ability of condensed matter physics to not
only to describe nature, but also to manipulate nature. We live in
one universe, but crystalline solids allow us to create or discover
another universe with different properties. Do you want a
universe where magnets only have a north pole, but no south
pole? This was realized inside so-called Pyrochlore materials,
which were synthesized in a lab and whose peculiar magnetic
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structure gives rise to quasiparticles, which behave like magnetic
monopoles [8]. Do you want a two-dimensional universe? Maybe
one with a slower speed of light—a slower cosmic speed limit?
Both are realized in graphene, a fantastical material which is
usually produced in the most mundane way possible: by taking a
piece of scotch tape to a hunk of graphite rock mined out of the
Condensed matter physics is simultaneously large and small . I
mean this both in terms of the experiments (and calculations)
that can be done and the science itself. Many experiments in
condensed matter physics can be performed on a tabletop by a
single student in a lab at a relatively low cost. Other experiments,
however, are performed at large user facilities such as
synchrotrons, neutron scattering research reactors and free
electron-lasers, which require a full time support team and can
cost more than a billion dollars to build (the good news is they
can be used for many different experiments, not only in
condensed matter physics, but in chemistry and biology too). On
the theoretical side of the field, some people do pencil and paper
calculations, while others apply for time on a supercomputer to
numerically study systems of many-interacting particles. The
science of condensed matter has a small number of tiny
constituents: electrons, protons, and neutrons. But when many,
many of them are put together, emergent properties can appear
that encompass a macroscopic material and are often quite
different from the sum of their parts.
And that brings me to the amazing phenomena that appear in
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condensed matter systems [10]. It should be noted that
oftentimes these phenomena are discovered by surprise, not
predicted beforehand. Previously, I discussed fractional charges
in the fractional quantum hall effect and superconductivity (fun
fact: the theory of the Higgs’ Boson originates from the theory
explaining why certain metals become superconductors at low
temperature; all of physics is connected). Other cool phenomena
include super-obese electrons in some rare-earth compounds who
behave as if they have a mass 1,000 times that of a free electron
[11], materials in which the resistance suddenly increases by a
factor of 100,000 when subjected to a magnetic field [12], highly
radioactive elements that undergo five different structural phase
transitions in their solid state [13], fractal behavior (Hofstadter's
butterfly) in graphene/boron nitride heterostructures, novel types
of magnetic order such as skyrmions (the name alone…), just to
name a few. And we are not limited to the phenomena we know
about today: the smallest speck of crystalline solid contains over a
septillian mutually interacting electrons and ions, which can be
arranged in nearly limitless ways, so there is no shortage of
astounding phenomena (some of which might be useful, too)
waiting to be discovered/invented. It goes down in the CM, for
sure.
A big thank you to Prof. Alexander F. Kemper, Dr. George
Burkhard, and Noah Raman for helpful suggestions,
improvements, and discussion on this piece.
Footnotes
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[1] Observation of Majorana fermions in ferromagnetic atomic
chains on a superconductor
[2] http://www.nature.com/nature/jou...
[3] http://www.nature.com/nphys/jour...
[4] High-temperature superconductivity
[5] http://www.nature.com/nature/jou...
[6] Iron Exposed as High-Temperature Superconductor
[7] https://arxiv.org/ftp/cond-mat/p...
[8] Dirac Strings and Magnetic Monopoles in the Spin Ice
Dy2Ti2O7
[12] Thousandfold Change in Resistivity in Magnetoresistive La-
Ca-Mn-O Films
[14] http://www.nature.com/nature/jou...
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