FEMTOTECH ATTOTECH XTECH

“SIPI” SEARCH FOR INFRA PARTICLE INTELLLIGENCE

DEIFYING PHYSICS

Prof. Dr. Hugo de GARIS profhugodegaris@yahoo.com http://profhugodegaris.wordpress.com

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 …

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

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?

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}

AN ANTI-QUARK HAS ONE OF THESE CHARGES {ANTI-RED, ANTI-GREEN, ANTI-BLUE}

GLUONS ARE LIKE PHOTONS, THEYBIND 3 QUARKS TOGETHER TO MAKE NUCLEONS (PROTONS, NEUTRONS)

GLUONS ARE BI-COLOR CHARGED

E.G.

RED & ANTI-BLUE, BLUE & ANTI-RED

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

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

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

1 1 1 1 0 1

0 1 1

0 0 0

1 1 1

1 0 0

0 1 0

0 0 0

1 0

0 1

A ~A

A B AvB

A B A&B

LOGIC GATES

NOT

OR

AND

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 !

THE GOAL NOW IS TO USE THE PROPERTIES OF QUARKS AND GLUONSTO 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

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

NOT GATE USING QUARKS AND GLUONS

FILL THE CHAMBER WITH TWO KINDS OF GLUONS Gr,~b and Gb,~r

Gr,~bGb,~r

Gr,~bGb,~r

Qr

QrQb

Qb

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

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.

GluonEmitting

Chamber A

QuarkChamber B

Qr(1) Gr,~b

Qr(2)

Qr

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.

GluonEmitting

Chamber A

QuarkChamber B

Qr(1) Gr,~b

Qb(2)

Qr

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.

GluonEmitting

Chamber A

QuarkChamber B

Qb(1) nothing

Qr(2)

Qr

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.

GluonEmitting

Chamber A

QuarkChamber B

Qb(1) nothing

Qb(2)

Qb

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.

AC

B

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).

There are only red quarks in chamber C, so only red quarks can exit chamber C. Output is Qr

Qr(1)

Qr(3)

Qr(2)

Qr

Qr Qr

AC

B

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).

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.

Qr(1)

Qr(3)

Qb(2)

Qb

Qr Gb,~r

AC

B

blue(1), red(2): (i.e. blue quarks(1) enter chamber A, and red quarks(2) enter chamber B). The blue quarksQb(1) that enter chamber A generate blue, anti-red gluons Gb,~r which pass into chamber C.

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.

Qb(1)

Qr(3)

Qr(2)

Qb

Gb,~r Qr

AC

B

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.

These gluons convert the fixed red quarks enteringchamber C to blue quarks, so that only blue quarks exit from chamber C.

Qb(1)

Qr(3)

Qb(2)

Qb

Gb,~r Gb,~r

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 HAVEA VERY SHORT RANGE, AN ATTOMETER.

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.

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

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

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

“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

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-

BY SUBSTITUTING THE COLORS OFTHE QUARKS FOR THEIR FLAVORS

AND SUBSTITUTING THE GLUONS FOR THE Ws

PRECISELY THE SAME LOGIC GATES CAN BE USED, SO WE HAVE ANATTOSCALE COMPUTING, WHICH ISTHE BEGINNINGS OF AN ATTOTECH

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.

HENCE A FEMTOLECT COULD VASTLY OUTPERFORM ITS NANOLECT COUSINS

THIS LOGIC APPLIES AT ANY LEVEL OF X-TECH, RIGHT DOWN TO PLANCK SCALEWHICH 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!!!

“SIPI”

SEARCH for INFRA PARTICLE INTELLIGENCE

THE MOST INTELLIGENT CREATURES IN THEUNIVERSE ARE PROBABLY TINY AND “LIVE” INSIDE ELEMENTARY PARTICLES.

SETI SHOULD MAKE WAY TO SOME EXTENT FOR SIPI.

HOW TO DETECT INTELLIGENCE INSIDE ELEMENTARY PARTICLES?

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”