Summary - Introduction to Evolutionary Computations. Akira Imada
The Higgs Boson: What is it? Have we found it
1. The
Higgs
Boson:
What
is
it?
Have
we
found
it?
Michael
Tuts
Columbia
University
Cambridge/MIT
Alumni
December
4,
2012
2. A
Journey
to
the
Domain
of
Par=cle
Physics
10-‐12
meter
1
m m eter
10-‐14eter
-‐2
-‐6
-‐1
-‐16
10 -‐9
-‐15 meter
-‐5
-‐3
-‐4
-‐7
-‐8
-‐13
meter
-‐11
-‐10
3
Carbon
A
Skinurface loud
Skin
White
uarks
lectrons
Within
Skin
tructure
roton
cCarbon
mersonn
ell
olored
onhucleusdetail
pAtomic
trandsp c
DNA
uter
e i
C
A
q elood
Cell
mpore
DNA
ucleus
ore
ipn and
nner
n
Proton’s
sucleus
DNA
sicro-‐organism
slectron
the
Bolecules
4. The
“Standard
Model”
of
Par=cle
Physics
Ordinary
maTer
(planets,
us!)
is
made
of
this
first
generaYon
of
quarks
and
leptons
5.
6. Very
heavy!
Very
light!
Massless!
Very
heavy!
Higgs
“mechanism”
provides
a
way
they
should
all
But
our
simplest
theory
would
s ay
to
explain
why
the
massless!
par=cles
have
different
weights
be
elementary
(masses)…
How?
9. How
can
we
answer
this
ques=on
–
does
the
Higgs
Boson
exist
and
can
we
prove
it?
The
Tools
for
explora=on
1.
Create
a
Higgs
in
the
debris
of
par=cle
collisions
–
use
the
Large
Hadron
Collider
2.
Search
for
the
Higgs
in
that
debris
–
use
the
ATLAS
detector
as
a
microscope
to
explore
the
subatomic
world
10.
11. Proton-‐proton
collisions
at
7TeV
per
beam
At
the
CERN
lab
in
Geneva
Switzerland
17mile
long
tunnel,
300
feet
underground,
1,200
magnets
12.
13.
14.
15. The
ATLAS
Detector
is
big,
very
big
• 80
c
tall,
147
c
long,
7,000
tons,
100
Million
channels
of
electronics
16. How
big
is
ATLAS?
…
very
• 100
million
channels
of
electronics
• 80
c
tall
• 140
c
long
• 7,000
tons
• 3,000
physicists
(incl.
~1,000
graduate
students)
• 38
countries
• 175
ins=tu=ons
17.
18. Think
of
the
ATLAS
detector
as
a
100
megapixel
digital
camera
• 100
million
channels
of
electronics
• We
take
electronic
“pictures”
(called
events)
• We
take
40
million
“pictures”
per
second
• We
analyze
these
“pictures”
using
a
worldwide
network
of
50,000
computers
• We
have
wrigen
already
~40
PB
of
data
(40,000,000
Gigabytes!)
LHC
#6
by
Jonathan
Feldschuh
(2008)
The
problem
• A
total
1
billion
collisions
per
second
• Most
are
“uninteres=ng”,
so
need
to
decide
and
discard
quickly,
can
only
afford
to
save
200
per
second
• For
example,
Z
boson
–
15
per
second
• For
example,
Higgs
boson
–
one
every
5
LHC
#26
by
Jonathan
Feldschuh
seconds
19. How
do
you
classify
“pictures”
as
interes=ng
or
less
interes=ng?
Can
you
tell
the
difference
between
these
two?
20. An
ATLAS
“Picture”
…
maybe
a
Higgs?
ZZ→e+e-‐µ+µ-‐
This
could
be
a
Higgs
event
…
or
more
mundane…
need
more
data
to
tell
for
sure
23. So
what
do
we
see
in
the
actual
data?
Combine
the
2
photons
according
to
Einstein’s
equa=ons
to
tell
us
the
weight
(mass)
of
the
parent
par=cle
For
mH=126.5
±
2
GeV:
observed:
3693
events
expected
from
B:
3635
expected
from
SM
Higgs:
100
Signal/Background
~
3%
1015
(=1,000,000,000,000,000)“pictures”
taken
Around
the
“bump”
about
3,700
“pictures”
of
which
about
100
correspond
to
the
new
par=cle
24.
25. If
it
is
Higgs
–
do
we
see
it
produced
at
the
rate
we
expect
from
theory?
26. Are
we
done
–
is
this
the
end?
No!
It
is
a
new
beginning!
This
is
not
“just”
a
new
par=cle
–
a
Higgs
would
be
unlike
any
we
have
ever
seen
before
Is
it
a
Higgs
Boson?
Not
completely
sure
yet…
Is
it
produced
as
ocen
as
we
expect?
Does
it
decay
as
we
expect?
Are
its
other
proper=es,
like
“spin”,
as
predicted?
So
far
looks
like
it
…
but
we
will
be
accumula=ng
even
more
data
27. It’s
not
just
Higgs!
The
stuff
we
are
made
of
–
the
Standard
Model
I
described
-‐
makes
up
a
mere
4%
of
the
universe
There
are
many
open
ques=ons
we
may
be
able
to
tackle…
What
is
dark
Mager?
Are
there
new
symmetries
and
par=cles?
What
is
the
nature
of
space-‐=me
itself?
Something
we
never
thought
of?
Exploring
this
new
energy
fron=er
is
like
Columbus
sesng
sail
across
the
Atlan=c
–
will
we
find
America,
India
or
a
new
con=nent?
28. People
Columbia
U• niversity
group
on
ATLAS
June
2012
– 38
countries
– 176
insYtuYons
(including
Cavendish,
Cambridge
U)
– 3,054
authors
• In
the
U.S.
– 43
insYtutes:
Albany,
ANL,
Arizona,
UT
Arlington,
Berkeley
LBL
and
UC,
Boston,
Brandeis,
BNL,
Chicago,
Columbia,
UT
Dallas,
Duke,
Fresno
State,
Hampton,
Harvard,
Indiana,
U
Iowa,
Iowa
State,
UC
Irvine,
Louisiana
Tech,
MassachuseTs,
MIT,
Michigan,
MSU,
New
Mexico,
NIU,
NYU,
Ohio
State,
Oklahoma,
Oklahoma
State,
Oregon,
Pennsylvania,
PiTsburgh,
UC
Santa
Cruz,
SLAC,
SMU,
South
Carolina,
SUNY
Stony
Brook,
Tuhs,
Illinois
Urbana,
Washington,
Wisconsin,
Yale
– 592
authors
30. Come
join
us
on
this
journey!
• If
you
are
in
kindergarten
or
beyond
we
will
need
you…become
a
parYcle
physicist
and
join
ATLAS!
• In
Geneva?
Come
visit
us
at
CERN
(hTp://outreach.web.cern.ch/outreach/visits/)
• Follow
us
on
TwiTer
(twiTer.com/ATLASexperiment),
Facebook
(
facebook.com/group.php?v=wall&gid=23271817589),
You
Tube
(
www.youtube.com/theATLASExperiment)
–
even
a
LHC
rap
video
(
youtube.com/watch?v=j50ZssEojtM),
Blogs
(uslhc.us
and
atlas.ch/blog/)
• Watch
events
live
as
they
are
collected
(atlanYs.cern.ch/live/)
• Want
to
learn
more?
Keep
your
ATLAS
pop-‐up
book
handy
(
hTp://www.facebook.com/pages/Pop-‐up-‐Voyage-‐to-‐the-‐Heart-‐of-‐MaTer/153102255147
)
as
you
navigate
the
ATLAS
website
www.atlas.ch
• Oh…and
we
even
have
a
line
of
ATLAS
clothing
and
cool
toys
–
caps,
fleeces,
Yes,
3D-‐viewers,
puzzles,
cards,…
(atlas.ch/store.html)
31.
32. …
but
the
Higgs
mechanism
leaves
us
another
puzzle
-‐
why
is
the
Higgs
so
light?
(“Hierarchy
problem”)
The
Fix:
-‐
either
very
finely
tuned
cancella=on
(just
luck!)
OR
-‐
introduce
a
new
idea
like
SUPERSYMMETRY
(SUSY)
The
Price:
-‐
double
the
number
of
elementary
par=cles,
none
of
which
have
been
seen!
33. The
Bonus:
-‐
Besides
“fixing”
problems
with
SM
-‐
It
might
be
that
the
lightest
SUSY
par=cle
is
dark
mager!
-‐
String
theories
require
them!
We
won’t
We
might
have
discove
much
r
this
at
to
say
the
LHC
about
this
This
is
us
(the
standard
model)
34. But
what
about
the
force
of
gravity?
…
It
wasn’t
in
our
Standard
Model
The
Problem
– We
know
how
it
behaves
at
large
distances
–
Einstein’s
Theory
of
General
Rela=vity
tells
us
how
– At
small
distances
quantum
theory
is
important
and
we
have
no
tested
theory
of
quantum
gravity
(for
all
they
other
forces
we
do
have
a
quantum
theory)
– Why
is
it
so
weak?
(is
it
weak?
You
can
do
the
demo
at
home!)
The
Solu=on…perhaps
– Maybe,
just
maybe,
String
Theory
or
string
theory
inspired
ideas
are
the
answer
Our
experimental
problem
– Do
we
have
any
hope
of
tes=ng
it?
37. • High-‐energy
proton
collisions
• Can
release
enough
energy
• To
create
new,
heavy
par=cles
'Children
learn
about
the
world
much
as
scienYsts
do-‐-‐smashing
things
to
smithereens,
staring
in
wonder
at
the
results
and
then
breaking
out
in
giggles’