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*
Introduction
This
report constitutes
a more detailed
account
of
the psychoenergetic
devices
and
experiments
investigated during
a recent A.R.E .
fact-finding trip
to Russia.
As
such,
it
is
an extension of
the General Technical Report^
written concerning
the
trip rather
than
a substitute report.
For
a complete
picture of
the information received during
this
trip,
both reports
are neces-
sary.
Since
it was
felt
that many people would
not be interested
in the
details of these devices
and experiments,
two
reports have been written.
The
present
report deals with
three topics:
(1)
Kirlian photography,
(2)
Acupuncture points
and
the Tobiscope
and
(3)
Telekinesis’ (PK)
experiments
and
field detectors,
® •
Technical Data
•
Kirlian Photography
In
this
area of investigation,
the
important device
factors
fall
into
two categories:
(a)
the operating characteristics of
the electrical power
source and
(b)
the configuration and components
of
the information display
and recording devices.
(a)
It was
indicated
that
the
power source should
be
a pulsed high-frequency
field
(somewhat
similar
to
a radar
power source).
The pulse characteristics
are given
in Fig.
and
are
(i)
pulse height
= 20-100Kvo lt,
(ii)
pulse width
1 0
to
x
10~ fl
sec,
(iii)
pulse repetition period =^50 sec
and
(iv)
A.C.
frequency -
to 3000KHertz.
They were of
the opinion
that
a single D.C.
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pulse would
not be effective
in producing
the effect*
[*Howevcr, work carried
out
in England using this
approach
has
revealed
very
interesting photographs
from radiation
in
the ultra-violet.]
They mentioned
that
it was dangerous
to
use D.C,
rather
than high
frequency; with high
frequency inside
the pulse enve-
lope,
one can work with
living systems.
Although
a static
electric
field
of
the same value
as
used
in
the A.C*
system
107
volts/cm)
would
also yield cold electron emission,
the situation
is
not straightforward
as strong polarization of
the electrodes would occur
(electroys is)
.
They
feel
that
it
is necessary
to have
a discharge spacing be-
tween
the specimen and
the
film in order
for
proper channel
formation
to
occur
(as
a result of positive
ion clustering around
the electron stream).
The
electrons
exit
from the surface with different velocities
and
this
includes
information about
the object.
If one uses
a D.C.
power source,
equilibration
few
of electrons occurs
and
the
image
is
absent.
With D.C.,
in
the
first/raoments
an image appears
but
then disappears
later
as
equilibration occurs.
The H.F,
signal
is
also
used
in
the pulse
so
that one can decrease the size of
the equip-
ment.
The use of different
frequencies
allows
one
to obtain quite different
•pictures,
presumably associated with different
resonances
frpm different cells,
etc.;
i.e.,
the electrons
can come
from different
parts of
the
skin.
Actually,
one need
use only one pulse
to obtain
a photograph.
The
slow
pulse repetition rate
is
to provide
low average
power.
It
seems
that
a pulse
duration of about
x
10~ 3
sec
is maximum and
if
t
is much larger,
the
image
is
poor.
On
the other hand,
if
t
is
too
small,
the channel discharge process
doesn't have
time
to develop
(for contact
photography,
one can use
t ^
x
1CT 6
sec)
.
The
tot al
current drawn
from
the entire surface
is
less
than
1^
amp
s o
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that
the actual current
in
a discharge channel
is much
less.
They
sur.g-
that
this
is
the reason
for
the stability of the cold
electron emission.
The average power of
a
generator
is
about
1 watt
(pulse power
is much
larger,
of course).
Thus,
quite small
generators using batteries,
transformers,
transistors,
etc,,
can be built
and
taken out
into
the
field.
However,
such
small
generators
generally
do not
have
as much stability
as one would
like.
It was
stated
that
any discharge
includes photons but
that only dis-
charges
in
a strong
field produce
an image.
This
seems
to relate
to electron
acceleration which
leads
to
photon emission.
Of course,
even
the radiation
damage effect of the electrons hitting
the photographic grains can be expected
to produce massive exposure of such grains.
(b)
In the simplest Kirlian device,
shaped
like
a sandwich or parallel
plate
condenser,
the object
is
placed between
the
two plates
to which voltage
is
applied.
If
the condenser plates
are
too close
to
the object,
there will
be
no effect on
the
film.
In order
to
get
good
pictures,
there must be
a die-
lectric gap between
the object
and
the
film.
The exposure
time depends on
the
film speed
and on
the power density of the electric
field.
*
To
improve
the effect
and augment
it,
a
fine screen
(like
a silk screen)
may be placed between
the object
and capacitor plate
(and
film)
.
The
film
is between
the condenser plate
and
the screen.
This
screen enhances
the
effect,
probably by
its
serving
as
a dielectric.
One
type of effective screen
material
is
film itself
that
has
been completely exposed
and developed.
The device can
be placed
in
a scissors arrangement
as
illustrated
in
Fig.
2,
the scissors being used
to
apply
a slight but even pressure via
the
paralon
(or
sponge)
pads.
The electrodes
are developed x-ray
film
(AgBr
-* Ag)
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and
the
leads
are
fastened
to
them as
indicated.
The dull matt
finish of
these electrodes
provides
poor reflectivity of
light
and
thus
is
an aid
to
producing
a
good
image.
The spacing between object
and
film
is
about
microns
(can be
10p,
to
lOOp,)
.
To
improve
the
resolution,
a
layer pf saline water
or other conductive
liquid
is sometimes
placed between
the object
and
the
film.
In
this
case,
the
film
is
placed with
the emulsion
facing away
from
the object
so
that
the
emulsion won't
be disturbed.
The capacitor plate
is
then placed outside of
the
film.
A
further improvement
can be made by using
the conductive
liquid
as one of
the capacitor plates,
thereby permitting better resolution and
faster work with
the
film.
For taking pictures of a section of human skin or other part of the body,
only one electrode
is
needed.
In
this ca^e,
the body acts
as
ground;
i.e.,
only one half of
the device,
presented
in Fig.
2,
is
needed.
This
same elec-
trode procedure
is
used
for
the Kirlian microscope,
illustrated
in Fig.
3,
when
it
is
applied
to
the body.
Photographs of
the one-electrode device
and
the microscope are shown
in Fig.
4.
A simple rolling device, which
has
the advantage of operating at
less
than
1 watt average
power, was
also described.
It
is
illustrated
in Fig.
5.
In
this device,
no discharge occurs
at points A or C
but does occur
at
point
B where
the spacing
is
about
10 microns.
The cylinder
is
rolled
at about
cm/inin and
gives
a moving line discharge
to expose
the
film
in sequence.
A device
for
taking moving pictures
is
illustrated
in
Fig.
6.
It utilizes
the arrangement of
Fig.
2.
Controlled weights
are applied
to
the device and
the
film
is
pulled
through at some particular speed while
the discharge
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process
is
going on.
The
film
is
rolled
in
the usual way and
all
is contained
within
a casette.
In Fig.
7,
an extremely useful device
idea
is
illustrated.
The previous
methods utilized rigid capacitor plates which do not allow one
to
take pictures
of objectshaving irregular profiles.
In
the new method
(described
• in Russian
patent #209968
filed
in
1966
by Adamenko
and
Kirlian)
,
the device
takes
the
shape of
the body.
The transparent electrode
is
a silicon organic
film;
how-
ever, many other possibilities
exist.
With
this device,
any portion of the
body can be photographed directly.
In
fact,
one could make
a snug-fitting
vest
or garment of
the material which could
then be monitored photographically
from
a distance or displayed continuously via closed -c ircuit
T.V.
This
new method
grew out of an earlier
idea of Kirlian 's
(patent #164906
in
1963) which utilized
a conductive
transparent material
as part of
the
capacitor,
to which
a hinged mirror was
attached,
and a flexible conductive
material which
is
laid
upon
the object
to be photographed.
The mirror
is
con-
cave
and
acts
as
a
lens,
enlarging
the object
to
be studied.
The mirror
Is
apparently used
for visual
examination when not
taking photographs.
Between
the object
and
the
flexible,
transparent
condenser plate
is
placed
a dielectric
net.
A photographic
plate
is
placed over
the
front
or
top of
the conductor
so
that
the prints were merely contact prints without
focusing.
The
foregoing devices
all operate
in air at
atmosphere pressure.
If
the pressure
is
reduced
to
10“ 5
mm of mercury,
the
image
is
still
retained
even with
the electrode separation increased
to 20-30
cm.
At
a pressure of
lO-6 mm of mercury,
the
image disappears.
A visual display system using
something
like
a
television tube
is
illustrated
in Fig.
8.
In
this CRT device,
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electrons
from
the object
impinge on
n
200p, -thick dielectric
film nnd
their
charge pattern induces charge polarization on
the other side of
the
film which,
in
turn,
affects
the preferential
geometry of electron emission
from the
film.
Thus,
the eventual
image on
the screen
is
indeed
that of
the object.
This
is
a very important phenomenon which allows many interesting modifications of
device design.
The methods have been developed
for
image amplification
(magnification)
.
In the
first
case,
they use cold emission obtained
in
the
small spacing device
(SOy.)
of Fig.
2 with
a high electric
field at
the edges,
~ 106 V/cm.
However,
E
is caused
to decrease
in
the middle
to E^ ~ 104 V/cm
(see Fig.
9a).
Thus,
the
magnification,
p, ,
is
given by
“
= k
C1>
They have obtained values
of
p, ~ 340.
The
second method
is
carried
out
in
a
CRT type device
as
illusti'ated
in Fig.
9b.
The short electrode
(cathode)
has
a
field
E1
and
the larger electrode
(anode)
has
a
field
E p
(E
~ 106 V/cm,
Ep
is
smaller)
.
In
this
case,
the magnification,
p,,
is
given by
Ei
S*
M-
Ep
“
S
'
( 2>
where
S
and
S
are
the
tensions of
the
two electrodes
(S, E,
» S„E„
from Gauss'
law and charge conservation)
Using
the T„V.
tube
type of device,
one might
expect
that
the use of
electron
lenses would allow one
to build
an electron microscope with very high
magnification.
However,
because of
the
high vacuum needed
in such
a device,
a severe limitation exists.
At
10“ 7
-
10“ p
mm of mercury pressure,
one
gets
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no
image because of the
loss of channeling
ions
but
at
10~ 4
-
mm Hg,
one
doesn't even need
a
lens.
[ The use of
the dielectric
imprinting technique
may be
a helpful
aid here.]
In concluding
this
section,
it was
noted
that,
if
a person's
finger-
grintS—were sanded off,
the Kirlian photographs
fstilll
rcvp.alp.d . .f.hn
qjJ-filpal
^fingerprint s
.
Li kewise,
if
to
10% of
a
leaf has
been cut away
from one
edge,
the
ent i.re_.xad.iat ion pattern of-
t
he unaltered
leaf was
still
revea 1 ed
VP
the K
i
ho-tagraplu—
[
It would be useful
to perform
the experiment
by cutting successive
strips
from
the
leaf and photographing
in order
to see
what percentage of
the
leaf can
be removed without
an alteration
in
the
total
radiation pattern.
Dr, Adamenko
suggested
that
the number of radiation sources
in
the
Leaf or
finger may be
so numerous
as
to produce sufficient redundancy
of ihfoimaLion
that,
if
a portion of
the
leaf or skin
is
removed,
the
lost
sources
do
not significantly disrupt
the multiple array pattern,
«
Acupuncture
and
the Tobiscope
Although
it was
not
possible
to obtain
a circuit design
for the Tobi-
scope described
in Ref.
1,
it
is
possible
to
piece
together conversational
information and .propose critical circuit design
features
from which
a
person,
skilled
in electronics,
could make
an
instrument.
Most
simply,
the device
is
a D,C.
amplifier with
a high
input
impedance
and
is battery powered.
Very
likely,
the external
skin impedance
is
arranged
to
be placed
in parallel with
the
input
impedance of
the Tobiscope,
Thus,
if
the skin impedance
is
reason-
ably
large,
the
total operating
input
impedance
is unaltered by
increasing
the skin path
length.
However,
if
a number of locations
are
found which
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produce shunting or short circuit paths of
low impedance,
then
the effective
input
impedance of
the device
is
significantly
lowered.
For contact with
such points,
the current
flowing through
the device will be greatly increased
and
the current
change (or voltage change)
may be multiplied by
the D.C,
ampli-
fier
to
a sufficient degree
to
light
a
bulb
in
the head of the device.
The
illumination of
this
light
signals
the location of
a shunting path or an
acupuncture point.
The* device operates
on
less
than
1 micro
amp
at
4 volts with
the
tran-
sistor D.C.
amplifier being very stable over
the voltage
range of
1.3
to
3.5
volts.
The
input
resistance
is
about 4-5
x
106
ohms
and
the device needs
dry
skin
to
be effective
in locating
the acupuncture network points
(wet,
salty
skin leads
to
surface shunt
paths)
.
It
is
found
that
a resistance of about
50, x
10^
ohms
exists between
these network points
and
that
the value
increases
—
--
>
greatly during sleep.
Th e equivalent
r o. s i s t a nc
e
—
a
ve r— fcha . -
s
ame
between
two non-network points
is
in
the
range ~10°
ohms.
At present,
they
are
investigating an alternating current device and
find
that very
interesting
effects
occvir
in the
region of
KH per second
(since one now
sees
the
imagi-
nary part of
the
impedance)
.
The D.C.
resistance between one acupuncture point
and
another
is
about
K0
for
two adjacent network points
and varies
slowly,
as
the distance be-
tween points
increases,
to
about
100
KQ.
The
same range of variation occurs
due
to emotional
change,
light stimulus,
etc.
The procedure here
is
to
use
( 2 )
a small current
and
a bridge balance method.
As
pointed out by Adamenko
,
in
the case of emotional
excitation
the points vary
in diameter
(as
revealed
by conductivity area)
and
there
is
the possibility of
the
areas overlapping
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one another
to
form high conductivity regions.
Again,
it must be emphasized
that measurements
are meaningful only on dry skin.
They have investigated
the variation of conductivity between
the network
points according
to
the patient's condition
in hypnonis
(see
Fig,
11),
The
conditions
or states of hypnosis
are
listed
along
the abscissa
as:
(1)
ordi-
nary state,
(2)
sleep with closed
eyes,
(3)
sleep with open eyes,
(4)
sugges-
tion of hallucinations,
(5)
"artificial
reincarnation",
(6)
work in "reincar-
nation
state.
The
four graphs
show variations
in
four
groups of subjects
ranging
from control
group A
(those not
hypno tizable)
through
B,
C
and
D
in
increasing order of hypno tizability
.
As
seen
from
the
graphs,
there exists
a
certain relationship between
the patient's hypnobility
and
the character of
conductivity variations.
In
the control
group,
no conductivity variation
has
been recorded which
indicates
the absence of emotional
reactions
to
the
hypnotist's words.
However,
in
the case ot ordinary emotional states,
these
patients
exhibit conductivity variations.
It
has
also
been discovered
that
a voltage signal
can be detected
be-
tween
two network points
provided
two different
types
of metals
are used
as
electrodes.
On dry skin,
using plated circular electrodes
of
to
7 mm diam-
eter,
a
Ni-Ag combination yielded
a potential difference of about
rav.
At
skin
locations where such
points
are absent,
the potential difference
is
close
to
zero.
Likewise,
between
two network points,
using the same electrode ma-
terial
(Ni-Ni or Ag-Ag, say)
,
the potential difference
is
again close
to zero.
It
is
sufficient
to plate cu
electrodes with Ni or Ag
(they use chrome-Ni
and
chrome -Ag)
,
Adamenko
finds
that,
the greater
the work function difference,
A'J'p
between
the electrode materials,
the greater
the voltage,
^V,
developed.
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They think that
this
is
a galvanic
cell
effect with
the channel
of meridian
between
the
two network points
acting
as
an electrolyte
(like
a Pb-Zn battery).
The current drawn
from
this
battery
is
about
10 micro -amps;
however,
this
current
level polarizes
the electrodes
so
they use an impedance
to reduce
the
current
level
to about
2 q, amps
and
then amplify
the signal
for display purposes.
In cases of emotional -volitive excitation,
the potential difference aV may
in-
crease up
to
100 millivolts.
Using parallel connections
between several
net-
work points,
the voltage obtained may
be
as high
as 0.5-1 volt
and
the current
accordingly
increased
up
to
some saturation
limit
(L
= 10^
for
pair,
I
=
18pA
for
pairs,
etc.).
They
feel
that
this high current drain could
be
dangerous
to
the body.
This
network potential difference has
been used
to
power
a
simple transistor
radio
and
a
small
toy vehicle.
They
find
that,
as
the electrode area,
A,
increases, the developed voltage,
V,
increases.
They also
find
that
an A.C.
pulse
is diminished
as
the
area of
the electrode
increases.
This
is
illustrated
in Fig.
as
a plot of V vs.
time;
it
probably represents
an averaging phenomenon, wherein
the A.C.
signal
arises only
at
the acupuncture point
(less
than
1 mm
in diameter)
in
the cen-
tral
region of
the electrode
and potential
averaging occurs.
In Fig.
13,
the dependence
of semiconductor properties
of acupuncture
points
on
the physiological
state of
the
internal organs connected with
these
points
is
given.
The vertical
scale shows
the difference
in resistance
(dR)
between symmetrical
points
in
the direct
and
reverse directions.
Each vertical
line represents
a particular acupuncture connection.
Curves
and
4:
"healer"
before
and after
treatment.
Curves
and
3:
"patient" before and
after
treat-
ment .
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To
fasten electrodes
to
a plant,
glue can be used.
To
fasten electrodes
to
humans,
around
the head
for example,
mi open helmet
is
used which contains
screw contact
electrodes
that
can
be moved
about
and brought
into
light
but
constant pressure contact.
An interesting testing or training device,
using
a cylindrical capacitor
of
the
type
illustrated
in Fig.
14, was mentioned.
One hand was
placed on
the
A^, casing grasping
the cylinder
in
a
1 natural way
(some acupuncture points
touch
the aluminum can).
The
thumb
and
forefinger of
the other hand hold
the central
contact
post
(acupuncture points
in
finger
touch
the silver-plated contact).
The capacitor
is
held
in
this way
for one minute of charging and
it
is
then
.
,
,
,
.
microammeter
discharged
through a/
yielding
a maximum signal
I
,
say.
Next,
charging again occurs
for one minute,
but
this
time
the
investigator
also men-
tally concentrates on charging
the capacitor.
The maximum discharge current
is
IR
,
say,
yielding
a
ratio
K =
Ip/]^
-
the greater
is
K,
the greater
is
the
ability
to use one
T s mind
in controlling
the energy body.
The imagination of
stress
(or actual muscle
tension)
or excitement during
this one-minute .period
can be used
to
alter
Ip
,
Using
a
30 microfrared capacitor,
the author
found
sw 10pA;
a
larger capacitor
(up
to
10,000 M,f)
would probably be
better.
This
*
simple device can
be
used
to study one's ability
to concentrate
and
focus
the
mind
and
by practice,
oneshould
be able
to
increase K significantly.
It was
stated
that Alla
V,
the PK performer,
is
able
to produce K =
9 without
too much
difficulty.
3 .
Telekinesis
(PK)
They
find
that
the placing of
a
film on Nelya
K's
head during
the PK
experiment
leads
to
the presence of
a large exposed
spot on the
film.
They
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also
find
that
film exposure occurs
if
the
film
is
placed
under
the object
used
in a PK experiment.
In addition,
the
film may
also
be exposed
after
the
experiment due
to
a residual charge of some sort on the object.
We heard
that
Nelya K actually caused
a
frog's
heart
to
stop
(and
that
it then could
not be
started again electrically).
We also
learned
that she can influence
the heart
rhythm of other people and can alter
their skin condition
so
as
to produce
a
burning
feeling on contact.
They have
found
that hypnosis can be used
to en-
hance PK abilities
and
that autogenic
training was
used
to help increase Alla V
PK abilities.
It was
also
stated
that Nelya K cannot
move objects
if
they are
in a vacuum and
that
after
the
levitation of
a small ball
in air,
an electro-
static charge of
5 x
ri
coulombs was
found on the ball
.
It was
not possible
to obtain any specific
information concerning
the
Sergeyev detector of pulsating magnetic
ffelds
in
the vicinity of the PK object
However,
it
is
likely
to
be
the detection of
a magnetic
field using
a sensing
element of
the barium titanate variety.
It was
learned
that
plants make
p.vqn
better-dptC Qtors of
the PK fields, when electrodes
are applied
to
two
acupunc
ture_points
of
the plant.
.,
Using
5 mm diameter electrodes of Ni and Ag,
they
obtain about
rav between
two points which
is
amplified.
During
a PK experi-
ment,
current pulses occur which change
from
5 mA ambient
to over
100
itA
at
the
pulse
peak
(see Fig.
15)
.
They have not
fully studied
the distribution of
field strength between
the operator and object during PK and
find
it
to
be
a difficult question.
The
field intensity does
increase
as one
reaches
the object
but probably
not
in
the radiation type mode
illustrated
in Fig.
16.
They don't know what
type of
field pattern exists on
the other side of
the object
and seem
to
think that
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the
force
is somehow -just manifest
in
the vicinity of the object without
tan-
gible intervening
field
linkages between
the operator and object.
In the case
of the rolling cylinder used
in
the PK experiments by Alla V, Adamenko
thinks
that
a charge dipole
forms,
as
illustrated
in Fig.
17, which gives
a moment
such
that one could move
the object
in either direction depending on how one
held his
hand.
[This
is not clear
to me either.]
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tube)
2.
Thread
I
3.
Upper half of housing
I
-
A*
Pin
for focusing
'5.
Thread
6.
Lower half of housing
7.
Two orifices
(0 4mm)
disposed one
in
front
of the other
8.
Rubber washer
9.
Contact
to
power source
10.
Metallic wire
(for protection against
circuit disruption because of water
evaporation)
11.
Thickening
in form of a ring
12.
Pressing nut,
freely revolving
•3
13.
Collars
14.
Thread
15.
Traverse
16.
Orifice 0 5mm
17.
Bottom of
the traverse
18.
Glass with thickness
0.6-1.0mra
19.
Glass with thickness
0.13-0. 14mm
20.
Chamber
(cell),
flooded by water
through
orifice
21.
8-12
times objective
22.
Bushing which carries objective
23.
Thread
(in accordance with microscope
tube thread)
Fig.
3.
Discharge
- optical housing
Fig.
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