Sunday, May 4, 2014

Mathematicians trace source of Rogers-Ramanujan identities, find algebraic gold


Mathematicians have found a framework
for the celebrated Rogers-Ramanujan
identities and their arithmetic
properties, solving another long-
standing mystery stemming from the work of
Indian math genius Srinivasa Ramanujan.
The findings, by mathematicians at Emory
University and the University of Queensland,
yield a treasure trove of algebraic numbers and
formulas to access them.

"Algebraic numbers are among the first
numbers you encounter in mathematics," says
Ken Ono, a number theorist at Emory "And yet,
it's surprisingly difficult to find functions that
return them as values in a uniform and
systematic way."

Ono is the co-author of the new findings,
along with S. Ole Warnaar of the University of
Queensland and Michael Griffin, an Emory
graduate student.

Ono announced the findings in April as a
plenary speaker at the Applications of
Automorphic Forms in Number Theory and
Combinatorics conference at Louisiana State
University. He will also present them as a
plenary speaker at the 2015 Joint Mathematics
Meetings, the largest mathematics meeting in
the world, set for January in San Antonio.
Warnaar, Griffin and others will give additional
talks on the findings during an invited special
session to accompany Ono's plenary address.
The most famous algebraic number of all is the
golden ratio, also known by the Greek letter
phi.

Many great works of architecture and art,
such as the Parthenon, are said to embody the
pleasing proportions of the golden ratio, which
is also seen in beautiful forms in nature.

Mathematicians, artists and scientists, from
ancient times to today have pondered the
qualities of phi, which is approximately equal
to 1.618, although its digits just keep on going,
with no apparent pattern.

"People studied the golden ratio before there
was a real theory of algebra," Ono says. "It
was a kind of prototype for algebraic
numbers."

Although no other algebraic units are as
famous as the golden ratio, they are of central
importance to algebra. "A fundamental
problem in mathematics is to find functions
whose values are always algebraic numbers,"
Ono says. "The famous Swiss mathematician
Leonhard Euler made some progress on this
problem in the 18th century. His theory of
continued fractions, where one successively
divides numbers in a systematic way, produces
some very special algebraic numbers like the
golden ratio. But his theory cannot produce
algebraic numbers which go beyond the stuff
of the quadratic formula that one encounters
in high school algebra."

Ramanujan, however, could produce such
numbers, and he made it look easy.
"Ramanujan has a very special, almost mythic,
status in mathematics," says Edward Frenkel, a
mathematician at the University of California,
Berkeley. "He had a sort of Midas touch that
seemed to magically turn everything into gold."
And the Rogers-Ramanujan identities are
considered among Ramanujan's greatest
legacies, adds Frenkel, a leading expert on the
identities.
"They are two of the most remarkable and
important results in the theory of q-series, or
special functions," says Warnaar, who began
studying the Rogers-Ramanujan identities
shortly after he encountered them while
working on his PhD in statistical mechanics
about 20 years ago.

Although originally discovered by L. J. Rogers
in 1894, the identities became famous through
the work of Ramanujan, who was largely self-
taught and worked instinctively.
In 1913, Ramanujan sent a letter from his
native India to the British mathematician G. H.
Hardy that included the two identities that
Rogers discovered and a third formula that
showed these identities are essentially modular
functions and their quotient has the special
property that its singular values are algebraic
integral units. That result came to be known as
the Rogers-Ramanujan continued fraction.
Hardy was astonished when he saw the
formulas. "I had never seen anything in the
least like this before," Hardy wrote. "A single
look at them is enough to show they could
only be written down by a mathematician of
the highest class. They must be true because
no one would have the imagination to invent
them."

"Ramanujan seemed to produce this result out
of thin air," Ono says.
Ramanujan died in 1920 before he could
explain how he conjured up the formulas.

"They have been cited hundreds of times by
mathematicians," Ono says. "They are used in
statistical mathematics, conformal field theory
and number theory. And yet no one knew
whether Ramanujan just stumbled onto the
power of these two identities or whether they
were fragments of a larger theory."
For nearly a century, many great
mathematicians have worked on solving the
mystery of where Ramanujan's formulas came
from and why they should be true.
Ono uses the analogy of going for a walk in a
creek bed and discovering a piece of gold. Had
Ramanujan accidentally found a random
nugget? Or was he drawn to that area because
he knew of a rich seam of gold nearby?

Warnaar was among those who pondered these
questions. "Just like digging for gold, in
mathematics it's not always obvious where to
look for a solution," he says. "It takes time
and effort, with no guarantee of success, but it
helps if you develop a lot of intuition about
where to look."
Finally, after 15 years of focusing almost
entirely on the Rogers-Ramanujan identities,

Warnaar found a way to embed them into a
much larger class of similar identities using
something known as representation theory.
"Ole found the mother lode of identities," Ono
says.
When Ono saw Warnaar's work posted last
November on arXiv.org, a mathematics-physics
archive, his eyes lit up.

"It just clicked," Ono recalls. "Ole found this
huge vein of gold, and we then figured out a
way to mine the gold. We went to work and
showed how to come full circle and make use
of the formulas. Now we can extract infinitely
many functions whose values are these
beautiful algebraic numbers."
"Historically, the Rogers-Ramanujan identities
have tantalized mathematicians," says George
Andrews, a mathematician at Penn State and
another top authority on the identities.

"They
have played an almost magical role in many
areas of math, statistical mechanics and
physics."

The collaboration of Warnaar, Ono and Griffin
"has given us a big picture of the general
setting for these identities, and deepened our
theoretical understanding for many of the
breakthroughs in this area of mathematics
during the past 100 years,"

Andrews says.

"They've given us a whole new set of tools to
be able to attack new problems."

"It's incredibly exciting to solve any problem
related to Ramanujan, he's such an important
figure in mathematics," Warnaar says. "Now
we can move on to more questions that we
don't understand. Math is limitless, and that's
fantastic."

Tuesday, February 25, 2014

The physics of curly hair: Researchers develop first detailed model for a 3-D strand of curly hair


Summary:

February 12, 2014
Massachusetts Institute of
Technology
The heroes and villains in animated films tend
to be on opposite ends of the moral spectrum.
But they're often similar in their hair, which is
usually extremely rigid or -- if it moves at all
-- is straight and swings to and fro. It's rare to
see an animated character with bouncy, curly
hair, since computer animators don't have a
simple mathematical means for describing it.
But now, researchers have developed the first
detailed model for a 3-D strand of curly hair.

FULL RESEARCH

The heroes and villains in animated films
tend to be on opposite ends of the moral
spectrum. But they're often similar in
their hair, which is usually extremely rigid
or -- if it moves at all -- is straight and swings
to and fro. It's rare to see an animated
character with bouncy, curly hair, since
computer animators don't have a simple
mathematical means for describing it.
However, change may be coming soon to a
theater near you: In a paper appearing in the
Feb. 13 issue of Physical Review Letters ,
researchers at MIT and the Université Pierre et
Marie Curie in Paris provide the first detailed
model for the 3-D shape of a strand of curly
hair.

This work could have applications in the
computer animation film industry, but it also
could be used by engineers to predict the
curve that long steel pipes, tubing, and cable
develop after being coiled around a spool for
transport. In the field, these materials often
act like a stubborn garden hose whose intrinsic
curves make it behave in unpredictable ways.

In engineering terminology, these items -- and
hair -- are all examples of a slender, flexible
rod.
Co-authors on the paper are Pedro Reis, an
assistant professor in MIT's Department of Civil
and Environmental Engineering and Department
of Mechanical Engineering; Basile Audoly and
Arnaud Lazarus, of the Université Pierre et
Marie Curie; and former MIT graduate student
James Miller, who is now a research associate
at Schlumberger-Doll Research. Miller worked
on this project as part of his doctoral thesis
research and is lead author of the paper.
"Our work doesn't deal with the collisions of
all the hairs on a head, which is a very
important effect for animators to control a
hairstyle," Reis says. "But it characterizes all
the different degrees of curliness of a hair and
describes mathematically how the properties
of the curl change along the arc length of a
hair."

When Reis set out to investigate the natural
curvature in flexible rods, he wasn't thinking
of hair. But as he studied several small flexible,
curved segments of tubing suspended from a
structure in his lab, he realized they weren't so
different from strands of curly hair hanging on
a head. That's when he contacted Audoly, who
had previously developed a theory to explain
the 2-D shape of human hair.
Using lab experimentation, computer
simulation, and theory -- "the perfect triangle
of science," Reis says -- the team identified the
main parameters for curly hair and simplified
them into two dimensionless parameters for
curvature (relating to the ratio of curvature
and length) and weight (relating to the ratio of
weight and stiffness). Given curvature, length,
weight, and stiffness, their model will predict
the shape of a hair, steel pipe, or Internet
cable suspended under its own weight.
As a strand of hair curls up from the bottom,
its 2-D hook grows larger until it reaches a
point where it becomes unstable under its own
weight and falls out of plane to become a 3-D
helix. Reis and co-authors describe the 3-D
curl as a localized helix, where only a portion
of the strand is curled, or a global helix, if the
curliness extends the entire length up to the
head.

A curl can change phase -- from 2-D to 3-D
local helix to 3-D global helix, and back again
-- if its parameters change. Because a strand
of hair is weighted from the bottom by gravity,
the top of the strand has more weight under it
than the tip, which has none. Thus, if the
weight on a hair is too great for its innate
curliness, the curl will fail and become either
straight or helical, depending on the strand's
length and stiffness.
For the curvature study, Miller created
flexible, thin rods using molds as small as a
bottle of Tabasco sauce and as large as the
columns in MIT's Lobby 7 (about a meter in
diameter). He injected a rubber-like material
inside hollow flexible tubing wrapped around
these molds. Once the rubber material cured
and the tubing was cut away, Miller and Reis
had flexible polyvinyl thin rods whose natural
curvature was based on the size of the object
around which they had been wrapped.

The researchers' use of dimensionless numbers
to describe innate curvature means the
equation will hold true at all scales. Even with
lengths measured in kilometers, the steel
piping used by the oil industry is flexible
enough to be spooled. "We think of steel pipes
as being nice and straight but usually at some
point they're getting wrapped around
something," Miller says. "And at large
dimensions, they're so flexible that it's like you
and I dealing with a limp spaghetti noodle."
"The mathematician [Leonhard] Euler first
derived the equation for a slender elastic body
-- like a hair strand -- in 1744," Audoly says.
"Even though the equations are well-known,
they have no explicit solution and, as a result,
it is challenging to connect these equations
with real shapes."
"The fact that I am bald and worked on this
problem for several years became a nice
running joke in our lab," Reis says. "But joking
aside, for me the importance of the work is
being able to take the intrinsic natural
curvature of rods into account for this class of
problems, which can dramatically affect their
mechanical behavior. Curvature can delay
undesirable instability that happens at higher
loads or torsion, and this is an effect that
engineers need to be able to understand and
predict."

Monday, February 24, 2014

NET / JRF IN MATHEMATICS

Council of Scientific and
Industrial Research
Human Resource
Development Group
Examination Unit

CSIR-UGC (NET) EXAM FOR AWARD
OF JUNIOR RESEARCH FELLOWSHIP
AND ELIGIBILITY FOR LECTURERSHIP

MATHEMATICAL SCIENCES

EXAM SCHEME
TIME: 3
HOURS
MAXIMUM M ARKS: 200

CSIR-UGC (NET) Exam for Award of
Junior Research Fellowship and
Eligibility for Lecturership shall be a
Single Paper Test having Multiple Choice
Questions (MCQs). The question paper
shall be divided in three parts.

Part 'A'

This part shall carry 20
questions pertaining to
General Science,
Quantitative Reasoning &
Analysis and Research
Aptitude. The candidates
shall be required to answer
any 15 questions. Each
question shall be of two
marks. The total marks
allocated to this section
shall be 30 out of 200.

Part 'B'

This part shall contain 40
Multiple Choice Questions
(MCQs) generally covering
the topics given in the
syllabus. A candidate shall
be required to answer any
25 questions. Each question
shall be of three marks. The
total marks allocated to this
section shall be 75 out of
200.

Part 'C'

This part shall contain 60
questions that are designed
to test a candidate's
knowledge of scientific
concepts and/or application
of the scientific concepts.
The questions shall be of
analytical nature where a
candidate is expected to
apply the scientific
knowledge to arrive at the
solution to the given
scientific problem. The
questions in this part shall
have multiple correct
options. Credit in a question
shall be given only on
identification of ALL the
correct options. No credit
shall be allowed in a
question if any incorrect
option is marked as correct
answer. No partial credit is
allowed. A candidate shall
be required to answer any
20 questions. Each question
shall be of 4.75 marks. The
total marks allocated to this
section shall be 95 out of
200.

· For Part ‘A’ and ‘B’
there will be Negative
marking @25% for each
wrong answer. No Negative
marking for Part ‘C’.

· To enable the
candidates to go through the
questions, the question
paper booklet shall be
distributed 15 minutes
before the scheduled time of
the exam. The Answer sheet
shall be distributed at the
scheduled time of the exam.
· On completion of the
exam i.e. at the scheduled
closing time of the exam, the
candidates shall be allowed
to carry the Question Paper
Booklet. No candidate is
allowed to carry the
Question Paper Booklet in
case he/she chooses to leave
the test before the scheduled
closing time.

· Model Question Paper
is available on HRDG
website www.csirhrdg.res.in