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FEMTOTECH ATTOTECH XTECH “SIPI” SEARCH FOR INFRA PARTICLE INTELLLIGENCE DEIFYING PHYSICS

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FEMTOTECH ATTOTECH

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Femtotech attotech

FEMTOTECH

ATTOTECH

XTECH

“SIPI”

SEARCH FOR

INFRA PARTICLE INTELLLIGENCE

DEIFYING PHYSICS

Prof. Dr. Hugo de GARIS

[email protected]

http://profhugodegaris.wordpress.com


Femtotech attotech

NANOTECH IS NOW WELL ESTABLISHED

NANOTECH IS WELL FUNDED

SO WHAT’S NEXT?

PICOTECH? (10-12 METER TECH)

NO!

BECAUSE NATURE PROVIDES NOTHING

AT THE PICO SCALE, SO …


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SO IT HAS TO BE FEMTOTECH

I.E. 10-15 METER TECH

I.E. THE SIZE OF NUCLEI,

OR NUCLEONS (PROTONS, NEUTRONS)

OR QUARKS

(3 QUARKS INSIDE A NUCLEON)

SO TO CREATE A FEMTOTECH, WE NEED

TO STUDY THE PROPERTIES OF QUARKS

AND THE GLUONS THAT BIND THEM


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THE MATHEMATICAL PHYSICS

STUDY OF QUARKS AND GLUONS

IS CALLED

“QCD”

QUANTUM CHROMO DYNAMICS

I.E. THE STUDY OF THE “COLOR FORCE”

WHAT IS COLOR?


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COLOR IS A FORM OF CHARGE

BOTH THE QUARKS AND THE

GLUONS ARE COLOR CHARGED

COLOR COMES IN 6 TYPES

RED, BLUE, GREEN

ANTI-RED, ANTI-BLUE, ANTI-GREEN

A QUARK HAS ONE OF THESE CHARGES

{RED, GREEN, BLUE}


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AN ANTI-QUARK HAS ONE

OF THESE CHARGES

{ANTI-RED, ANTI-GREEN, ANTI-BLUE}

GLUONS ARE LIKE PHOTONS, THEY

BIND 3 QUARKS TOGETHER TO MAKE

NUCLEONS (PROTONS, NEUTRONS)

GLUONS ARE BI-COLOR CHARGED

E.G.

RED & ANTI-BLUE, BLUE & ANTI-RED


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EMISSION OF A GLUON FROM A QUARK

A QUARK CAN EMIT A GLUON

E.G. A RED QUARK CAN EMIT A

RED & ANTI-BLUE GLUON, AND

THUS BECOME A BLUE QUARK

I.E. COLOR CHARGE IS CONSERVED

Qred  Qblue + Gred,anti-blue


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A QUARK CAN ALSO ABSORB A GLUON

E.G. A RED QUARK CAN ABSORB A

BLUE & ANTI-RED GLUON AND

THUS BECOME A BLUE QUARK

Qred + Gblue,anti-red  Qblue

I.E. COLOR CHARGE IS CONSERVED

THUS GLUONS CAN CHANGE

THE COLOR OF A QUARK


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WE NOW HAVE THE INGREDIENTS

FOR A FEMTOSCALE COMPUTING

BASIC IDEAS:

A) USE THE COLORS, RED AND BLUE

TO REPRESENT A “BIT” ON A QUARK

B) USE THE APPROPRIATE GLUONS TO

CHANGE THE COLOR OF A QUARK

I.E. TO “FLIP THE BIT” 1 => 0, 0 => 1


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LOGIC GATES

A ~A

A B A&B

NOT

AND

A B AvB

OR


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THERE IS A FAMOUS THEOREM IN

COMPUTER SCIENCE THEORY THAT

SAYS THAT THE SET OF LOGIC GATES

{NOT, OR, AND} IS COMPUTATIONALLY

UNIVERSAL

I.E. ANY BOOLEAN FUNCTION

DETECTOR CAN BE CONSTRUCTED

FROM THESE 3 LOGIC GATES

SO, LET’S MAKE THESE 3 GATES FROM

QUARKS AND GLUONS !


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THE GOAL NOW IS TO USE THE

PROPERTIES OF QUARKS AND GLUONS

TO BEHAVE LIKE THESE 3 LOGIC GATES

THE OUTPUT OF ONE LOGIC GATE

CAN BE FED INTO THE INPUT OF

ANOTHER LOGIC GATE

WE CAN THUS BUILD COMPUTERS

FROM THESE 3 LOGIC GATES


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A USEFUL FICTITIOUS DIDACTIC DEVICE

THE “QUARK CHAMBER”

PERHAPS A SPHERE THE SIZE

OF A NUCLEON

A QUARK ENTERS THE CHAMBER AT

ONE END AND EXITS AT THE OTHER END

AT THE SAME TIME, A GLUON MAY

ALSO ENTER THE CHAMBER


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NOT GATE USING QUARKS AND GLUONS

FILL THE CHAMBER WITH TWO

KINDS OF GLUONS Gr,~b and Gb,~r

Qr

Qb

Gr,~b

Gb,~r

Gr,~b

Gb,~r

Qb

Qr


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OR GATE, USES TWO CHAMBERS A & B

Chamber A is a gluon generating chamber.

If a red quark enters chamber A,

a red, anti-blue gluon Gr,~b emission is caused

in the chamber and the gluon then exits.

(The resulting blue quark is ignored.)

If a blue quark enters chamber A, nothing happens.

No gluon exits the chamber.

WE NOW HAVE 4 CASES


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red(1), red(2): (i.e. a red quark(1) enters chamber

A, and a second red quark(2) enters chamber B).

The red quark Qr(1) entering chamber A generates

a Gr,~b gluon that enters chamber B.

This gluon has no effect on the red Qr(2) entering

chamber B at the same time. The red Qr(2) then

passes out of chamber B unaffected. Output is Qr.

Gluon

Emitting

Chamber A

Quark

Chamber B

Qr

Qr(1)

Gr,~b

Qr(2)


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red(1), blue(2): (i.e. a red quark(1) enters chamber

A, and a blue quark(2) enters chamber B).

The red quark Qr(1) entering chamber A generates

a Gr,~b gluon that enters chamber B.

The blue quark Qb(2) that enters chamber B is

converted to a red quark Qr(2) that then exits

chamber B. . Output is Qr.

Gluon

Emitting

Chamber A

Quark

Chamber B

Qr

Qr(1)

Gr,~b

Qb(2)


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blue(1), red(2): (i.e. a blue quark(1) enters chamber

A, and a red quark(2) enters chamber B).

The blue quark Qb(1) entering chamber A generates

NO gluon, so no gluon enters chamber B.

The red quark Qr(2) that enters chamber B then

exits unchanged. In other words, the output quark

from chamber B is red. Output is Qr.

Gluon

Emitting

Chamber A

Quark

Chamber B

Qr

Qb(1)

nothing

Qr(2)


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blue(1), blue(2): (i.e. a blue quark(1) enters chamber

A, and a second blue quark(2) enters chamber B).

The blue quark Qb(1) entering chamber A generates

NO gluon, so no gluon enters chamber B.

The blue quark Qb(2) that enters chamber B then

exits chamber B unchanged. In other words, the

output quark from chamber B is blue. Output is Qb.

Gluon

Emitting

Chamber A

Quark

Chamber B

Qb

Qb(1)

nothing

Qb(2)


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AND GATE

The AND gate contains 3 chambers, A, B, C.

Chambers A and B both output a red quark if the

input is a red quark, and a blue, anti-red gluon Gb,~r

if the input is a blue quark.

This time, instead of dealing with single events,

think in terms of a stream of input and output quarks.

Chamber C has as input, the outputs of chambers

A and B, as well as a fixed red quark Qr(3) input.


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red(1), red(2): (i.e. red quarks(1) enter chamber A,

and red quarks(2) enter chamber B). The red quarks

Qr(1) and Qr(2) pass unchanged into chamber C,

along with the fixed red quarks Qr(3).

Qr(3)

A

B

Qr(1)

Qr(2)

C

Qr

Qr

Qr

There are only red quarks in chamber C, so only

red quarks can exit chamber C. Output is Qr


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red(1), blue(2): (i.e. red quarks(1) enter chamber A,

and blue quarks(2) enter chamber B). The red quarks

Qr(1) pass unchanged into chamber C, along with

the fixed red quarks Qr(3).

Qr(3)

A

B

Qr(1)

Qb(2)

C

Qr

Gb,~r

Qb

The blue quarks Qb(2) that enter chamber B generate

blue, anti-red gluons Gb,~r passing into chamber C,

converting all the red quarks in chamber C to blue

quarks, so that only blue quarks exit from chamber C.


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blue(1), red(2): (i.e. blue quarks(1) enter chamber A,

and red quarks(2) enter chamber B). The blue quarks

Qb(1) that enter chamber A generate blue, anti-red

gluons Gb,~r which pass into chamber C.

Qr(3)

A

B

Qb(1)

Qr(2)

C

Gb,~r

Qr

Qb

The red quarks Qr(2) that enter chamber B pass

unchanged into chamber C, along with the fixed red

quarks Qr(3). The gluons convert all the red quarks

in chamber C to blue quarks, that exit chamber C.


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blue(1), blue(2): (i.e. blue quarks(1) enter chamber

A, and blue quarks(2) enter chamber B). The blue

quarks Qb(1) and Qb(2) both generate blue, anti-red

gluons Gb,~r which pass into chamber C.

Qr(3)

A

B

Qb(1)

Qb(2)

C

Gb,~r

Gb,~r

Qb

These gluons convert the fixed red quarks entering

chamber C to blue quarks, so that only blue quarks

exit from chamber C.


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ATTOTECH

i.e. 10-18 METER TECH

THERE ARE 3 WEAK FORCE PARTICLES

W+, W-, Z0

UNLIKE PHOTONS AND GLUONS,

THESE FORCE GENERATING PARTICLES

HAVE MASS, A LOT OF MASS, SO HAVE

A VERY SHORT RANGE, AN ATTOMETER.


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FOR ATTOTECH COMPUTING, WE USE

ONLY THE W+ AND W-

THESE W PARTICLES CAN CHANGE THE

FLAVOR OF A QUARK.

QUARKS COME IN 6 DIFFERENT

FLAVORS (I.E. TYPES) UP, DOWN,

STRANGE, CHARMED, TOP, BOTTOM

A PROTON CONSISTS OF 2 UP QUARKS

AND 1 DOWN QUARK.


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AN UP (DOWN) QUARK HAS AN ELECTRONIC

CHARGE OF +2/3 (-1/3)

HENCE THE TOTAL ELECTRONIC CHARGE

OF A PROTON IS 2(+2/3) + 1(-1/3) = 3/3 = 1

A NEUTRON CONSISTS OF 1 UP QUARK,

AND 2 DOWN QUARKS

HENCE THE TOTAL ELECTRONIC CHARGE

OF A NEUTRON IS 1(+2/3) + 2(-1/3) = 0/3 = 0


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A W+ PARTICLE CAN CHANGE THE

FLAVOR OF A DOWN QUARK TO AN

UP QUARK

AND A W- PARTICLE CAN CHANGE THE

FLAVOR OF A UP QUARK TO A

DOWN QUARK

THUS WE CAN USE ALL THIS TO PERFORM

ATTOMETER SCALE COMPUTATION

HENCE THE BEGINNINGS OF ATTOTECH


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WE NOW HAVE THE INGREDIENTS

FOR AN ATTOSCALE COMPUTING

BASIC IDEAS:

A) USE THE FLAVORS, UP AND DOWN

TO REPRESENT A “BIT” ON A QUARK

B) USE THE APPROPRIATE W+ OR W- TO

CHANGE THE FLAVOR OF A QUARK

I.E. TO “FLIP THE BIT” 1 => 0, 0 => 1


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“X-TECH”

FROM NANOTECH TO FEMTOTECH

TO ATTOTECH, ETC

WHAT DO ALL THESE “TECHS” HAVE IN

COMMON FOR COMPUTING?

ANSWER:

THEY HAVE “STABLE” BINARY STATES

AND MECHANISMS TO FLIP THOSE BINARY

STATES BACK AND FORTH


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FOR FEMTOTECH

THE BINARY STATES ARE:

THE RED OR BLUE COLOR ON THE QUARK

THE STATE FLIPPERS ARE:

THE GLUONS Gr,~b and Gb,~r

FOR ATTOTECH

THE BINARY STATES ARE:

THE UP OR DOWN FLAVOR ON THE QUARK

THE STATE FLIPPERS ARE:

THE W PARTICLES W+ and W-


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BY SUBSTITUTING THE COLORS OF

THE QUARKS FOR THEIR FLAVORS

AND SUBSTITUTING THE GLUONS

FOR THE Ws

PRECISELY THE SAME LOGIC GATES

CAN BE USED, SO WE HAVE AN

ATTOSCALE COMPUTING, WHICH IS

THE BEGINNINGS OF AN ATTOTECH


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THESE “X-TECHS” PROVIDE AN ANSWER

TO “FERMI’S PARADOX”

WHICH IS :- “IF INTELLIGENT CREATURES

ARE COMMON PLACE IN THE UNIVERSE,

THEN “WHERE ARE THEY?”

A “FEMTOLECT” (I.E. A FEMTOSCALE

ARTILECT (ARTIFICIAL INTELLECT,

MASSIVELY INTELLIGENT MACHINE)

WOULD OUTPERFORM A “NANOLECT”

BY A FACTOR OF A TRILLION TRILLION.


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HENCE A FEMTOLECT COULD VASTLY

OUTPERFORM ITS NANOLECT COUSINS

THIS LOGIC APPLIES AT ANY LEVEL OF

X-TECH, RIGHT DOWN TO PLANCK SCALE

WHICH IS 10-35 METER.

SO IT IS THEN PROBABLE THAT THE

HYPER INTELLIGENT CIVILIZATIONS IN

THE UNIVERSE THAT ARE BILLIONS OF

YEARS OLDER THAN WE ARE, ARE ALL

AROUND US, TOO TINY FOR US TO

DETECT!!!


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“SIPI”

SEARCH for INFRA PARTICLE INTELLIGENCE

THE MOST INTELLIGENT CREATURES IN THE

UNIVERSE ARE PROBABLY TINY AND “LIVE”

INSIDE ELEMENTARY PARTICLES.

SETI SHOULD MAKE WAY TO SOME EXTENT

FOR SIPI.

HOW TO DETECT INTELLIGENCE INSIDE

ELEMENTARY PARTICLES?


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DEIFICATION OF PHYSICS

IF THIS ANSWER TO FERMI’S PARADOX IS

VALID, IT CHANGES THE WAY ONE LOOKS

AT (PARTICLE) PHYSICS.

X-LECTS WOULD HAVE GOD LIKE ABILITIES,

VAST INTELLIGENCES, PERFORMING AT

SPEEDS HUGELY SUPERIOR TO OURS.

THEY MAY HAVE ARRANGED THE

PROPERTIES OF THE UNIVERSE TO SUIT

THEMSELVES, MAKING IT “PROTONIC”


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