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Thermonuclear weapon
The basics of the Teller–Ulam design for a thermonuclear
weapon. Radiation from a primary fission bomb compresses a
secondary section containing both fission and fusion fuel. The
compressed secondary is heated from within by a second fission
explosion.
A thermonuclear weapon is a nuclear weapon that uses
the energy from a primary nuclear fission reaction to com-
press and ignite a secondary nuclear fusion reaction. The
result is greatly increased explosive power when com-
pared to single-stage fission weapons. It is colloquially re-
ferredto as a hydrogen bomb or H-bomb because it em-
ploys hydrogen fusion. The fission stage in such weapons
is required to cause the fusion that occurs in thermonu-
clear weapons.
[1]
The concept of the thermonuclear weapon was first devel-
oped and used in 1952 and has since been employed by
most of the world’s nuclear weapons.[2] The modern de-
sign of all thermonuclear weapons in the United States is
known as the Teller-Ulam configuration for its two chief
contributors, Edward Teller and Stanislaw Ulam, who de-
veloped it in 1951[3] for the United States, with certain
concepts developed with the contribution of John von
Neumann. The first test of a hydrogen bomb prototype
was the "Ivy Mike" nuclear test in 1952, conducted by
the United States. The first ready-to-use thermonuclear
bomb "RDS-6s" (“Joe4”) was tested on August 12, 1953,
in the Soviet Union. Similar devices were developed bythe United Kingdom, China, and France.
As thermonuclear weapons represent the most efficient
design for weapon energy yield in weapons with yields
above 50 kilotons, virtually all the nuclear weapons de-
ployed by the five nuclear-weapon states under the NPT
today are thermonuclear weapons using the Teller–Ulam
design.[4]
The essential features of the mature thermonuclear
weapon design, which officially remained secret for
nearly three decades, are:
1. Separation of stages into a triggering “primary” ex-
plosive and a much more powerful “secondary” ex-
plosive.
2. Compression of the secondary by X-rays coming
from nuclear fission in the primary, a process called
the "radiation implosion" of the secondary.
3. Heating of the secondary, after cold compression,
by a second fission explosion inside the secondary.
The radiation implosion mechanism is a heat engine
that exploits the temperature difference between the sec-
ondary stage’s hot, surrounding radiation channel and
its relatively cool interior. This temperature difference
is briefly maintained by a massive heat barrier called
the “pusher”, which also serves as an implosion tamper,
increasing and prolonging the compression of the sec-
ondary. If made of uranium, as is almost always the case,
it can capture neutrons produced by the fusion reaction
and undergo fission itself, increasing the overall explo-
sive yield. In many Teller–Ulam weapons, fission of thepusher dominates the explosion and produces radioactive
fission product fallout.
1
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3
inducing additional fission. Generally, a research pro-
gram with the capacity to create a thermonuclear bomb
has already mastered the ability to engineer boosted fis-
sion. When fired, the plutonium-239 (Pu-239) and/or
uranium-235 (U-235) core would be compressed to a
smaller sphere by special layers of conventional high ex-
plosives arranged around it in an explosive lens pattern,initiating the nuclear chain reaction that powers the con-
ventional “atomic bomb”.
The secondary is usually shown as a column of fu-
sion fuel and other components wrapped in many layers.
Around the column is first a “pusher-tamper”, a heavy
layer of uranium-238 (U-238) or lead which serves to
help compress the fusion fuel (and, in the case of ura-
nium, may eventually undergo fission itself). Inside this
is the fusion fuel itself, usually a form of lithium deu-
teride, which is used because it is easier to weaponize
than liquified tritium/deuterium gas (compare the suc-
cess of the cryogenic deuterium-based Ivy Mike exper-iment to the (over)success of the lithium deuteride-based
Castle Bravo experiment). This dry fuel, when bom-
barded by neutrons, produces tritium, a heavy isotope of
hydrogen which can undergo nuclear fusion, along with
the deuterium present in the mixture. (See the article on
nuclear fusion for a more detailed technical discussion of
fusion reactions.) Inside the layer of fuel is the “spark
plug”, a hollow column of fissile material (plutonium-239
or uranium-235) which, when compressed, can itself un-
dergo nuclear fission (because of the shape, it is not a
critical mass without compression). The tertiary, if one is
present, would be set below the secondary and probablybe made up of the same materials.[8][9]
Separating the secondary from the primary is the
interstage. The fissioning primary produces four types
of energy: 1) expanding hot gases from high explo-
sive charges which implode the primary; 2) superheated
plasma that was originally the bomb’s fissile material and
its tamper; 3) the electromagnetic radiation; and 4) the
neutrons from the primary’s nuclear detonation. The
interstage is responsible for accurately modulating the
transfer of energy from the primary to the secondary.
It must direct the hot gases, plasma, electromagnetic ra-
diation and neutrons toward the right place at the righttime. Less than optimal interstage designs have resulted
in the secondary failing to work entirely on multiple shots,
known as a “fissile fizzle”. The Koon shot of Operation
Castle is a good example; a small flaw allowed the neu-
tron flux from the primary to prematurely begin heating
the secondary, weakening the compression enough to pre-
vent any fusion.
Classified paper by Teller and Ulam on March 9, 1951:
On Heterocatalytic Detonations I: Hydrodynamic Lenses
and Radiation Mirrors , in which they proposed their
revolutionary staged implosion idea. This declassified
version is extensively redacted.
There is very little detailed information in the open lit-
erature about the mechanism of the interstage. One of
the best sources is a simplified diagram of a British ther-
monuclear weapon similar to the American W80 war-
head. It was released by Greenpeace in a report titled
“Dual Use Nuclear Technology” .[10] The major compo-
nents and their arrangement are in the diagram, though
details are almost absent; what scattered details it does
include, likely have intentional omissions and/or inaccu-
racies. They are labeled “End-cap and Neutron Focus
Lens” and “Reflector Wrap"; the former channels neu-
trons to the U-235/Pu-239 Spark Plug while the latter
refers to an X-ray reflector; typically a cylinder made out
of an X-ray opaque material such as uranium with the
primary and secondary at either end. It does not reflect
like a mirror; instead, it gets heated to a high temper-
ature by the X-ray flux from the primary, then it emits
more evenly spread X-rays which travel to the secondary,
causing what is known as radiation implosion. In Ivy
Mike, gold was used as a coating over the uranium to en-
hance the blackbody effect.[11] Next comes the “Reflec-
tor/Neutron Gun Carriage”. The reflector seals the gap
between the Neutron Focus Lens (in the center) and the
outer casing near the primary. It separates the primaryfrom the secondary and performs the same function as
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4 3 COMPRESSION OF THE SECONDARY
the previous reflector. There are about six neutron guns
(seen here from Sandia National Laboratories[12]) each
poking through the outer edge of the reflector with one
end in each section; all are clamped to the carriage and
arranged more or less evenly around the casing’s circum-
ference. The neutron guns are tilted so the neutron emit-
ting end of each gun end is pointed towards the centralaxis of the bomb. Neutrons from each neutron gun pass
through and are focused by the neutron focus lens towards
the centre of primary in order to boost the initial fission-
ing of the plutonium. A "Polystyrene Polarizer/Plasma
Source” is also shown (see below).
The first U.S. government document to mention the in-
terstage was only recently released to the public promot-
ing the 2004 initiation of the Reliable Replacement War-
head Program. A graphic includes blurbs describing the
potential advantage of a RRW on a part by part level,
with the interstage blurb saying a new design would re-
place “toxic, brittle material” and “expensive 'special' ma-terial... [which require] unique facilities”.[13] The “toxic,
brittle material” is widely assumed to be beryllium, which
fits that description and would also moderate the neutron
flux from the primary. Some material to absorb and re-
radiate the X-rays in a particular manner may also be
used.[14]
The “special material” is thought to be a substance called
"FOGBANK", an unclassified codename, though it is of-
ten referred to as "THE fogbank” (or "A Fogbank”) as
if it were a subassembly instead of a material. Its com-
position is classified, though aerogel has been suggested
as a possibility. Manufacture stopped for many years;however, the Life Extension Program required it to start
up again – Y-12 currently being the sole producer (the
“unique facility” referenced). The manufacturing process
used acetonitrile as a solvent, which led to at least three
evacuations in 2006. Acetonitrile is widely used in the
petroleum and pharmaceutical industries. Like most sol-
vents, it is flammable and can be toxic.[15]
2.1 Summary
A simplified summary of the above explanation is:
1. An implosion assembly type of fission bomb is ex-
ploded. This is the primary stage. If a small amount
of deuterium/tritium gas is placed inside the pri-
mary’s core, it will be compressed during the explo-
sion and a nuclear fusion reaction will occur; the re-
leased neutrons from this fusion reaction will induce
further fission in the plutonium-239 or uranium-235
used in the primary stage. The use of fusion fuel
to enhance the efficiency of a fission reaction is
called boosting. Without boosting, a large portion of
the fissile material will remain unreacted; the Little
Boy and Fat Man bombs had an efficiency of only1.4% and 17%, respectively, because they were un-
boosted.
2. Energy released in the primary stage is transferred
to the secondary (or fusion) stage. The exact mech-
anism whereby this happens is secret. This energy
compresses the fusion fuel and sparkplug; the com-
pressed sparkplug becomes critical and undergoes
a fission chain reaction, further heating the com-
pressed fusion fuel to a high enough temperature toinduce fusion, and also supplying neutrons that react
with lithium to create tritium for fusion.
3. The fusion fuel of the secondary stage may be sur-
rounded by depleted uranium or natural uranium,
whose U-238 is not fissile and cannot sustain a chain
reaction, but which is fissionable when bombarded
by the high-energy neutrons released by fusion in
the secondary stage. This process provides consid-
erable energy yield (as muchas half of the total yield
in large devices), but is not considered a tertiary
“stage”. Tertiary stages are further fusion stages (seebelow), which have been only rarely used, and then
only in the most powerful bombs ever made.
Thermonuclear weapons may or may not use a boosted
primary stage, use different types of fusion fuel, and
may surround the fusion fuel with beryllium (or another
neutron reflecting material) instead of depleted uranium
to prevent early premature fission from occurring before
the secondary is optimally compressed.
3 Compression of the secondary
The basic idea of the Teller–Ulam configuration is that
each “stage” would undergo fission or fusion (or both)
and release energy, much of which would be transferred
to another stage to trigger it. How exactly the energy is
“transported” from the primary to the secondary has been
the subject of some disagreement in the open press, but
is thought to be transmitted through the X-rays which are
emitted from the fissioning primary. This energy is then
used to compress the secondary. The crucial detail of
how the X-rays create the pressure is the main remainingdisputed point in the unclassified press. There are three
proposed theories:
• Radiation pressure exerted by the X-rays. This was
the first idea put forth by Howard Morland in the
article in The Progressive.
• X-rays creating a plasma in the radiation case’s filler
(a polystyrene or "FOGBANK" plastic foam). This
was a second idea put forward by Chuck Hansen and
later by Howard Morland.
• Tamper/Pusher ablation. This is the concept best
supported by physical analysis.
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3.3 Tamper-pusher ablation 5
3.1 Radiation pressure
The radiation pressure exerted by the large quantity of X-
ray photons inside the closed casing might be enough to
compress the secondary. Electromagnetic radiation such
as X-rays or light carries momentum and exerts a force
on any surface it strikes. The pressure of radiation at theintensities seen in everyday life, such as sunlight striking
a surface, is usually imperceptible, but at the extreme in-
tensities found in a thermonuclear bomb the pressure is
enormous.
For two thermonuclear bombs for which the general size
and primary characteristics are well understood, the Ivy
Mike test bomb and the modern W-80 cruise missile war-
head variant of the W-61 design, the radiation pressure
was calculated to be 73 million bar (atmospheres) (7.3 T
Pa) for the Ivy Mike design and 1,400 million bar (140
TPa) for the W-80.[16]
3.2 Foam plasma pressure
Foam plasma pressure is the concept which Chuck
Hansen introduced during the Progressive case, based
on research which located declassified documents listing
special foams as liner components within the radiation
case of thermonuclear weapons.
The sequence of firing the weapon (with the foam) would
be as follows:
1. The high explosives surrounding the core of the pri-mary fire, compressing the fissile material into a
supercritical state and beginning the fission chain re-
action.
2. The fissioning primary emits X-rays, which “re-
flect” along the inside of the casing, irradiating the
polystyrene foam.
3. The irradiated foam becomes a hot plasma, pushing
against the tamper of the secondary, compressing
it tightly, and beginning the fission reaction in the
spark plug.
4. Pushed from both sides (from the primary and the
spark plug), the lithium deuteride fuel is highly
compressed and heated to thermonuclear temper-
atures. Also, by being bombarded with neutrons,
each lithium−6 atom splits into one tritium atom
and one alpha particle. Then begins a fusion reac-
tion between the tritium and the deuterium, releas-
ing even more neutrons, and a huge amount of en-
ergy.
5. The fuel undergoing the fusion reaction emits a large
flux of neutrons, which irradiates the U-238 tamper
(or the U-238 bomb casing), causing it to undergoa fission reaction, providing about half of the total
energy.
This would complete the fission-fusion-fission sequence.
Fusion, unlike fission, is relatively “clean”—it releases en-
ergy but no harmful radioactive products or large amounts
of nuclear fallout. The fission reactions though, especially
the last fission reaction, release a tremendous amount of
fission products and fallout. If the last fission stage is
omitted, by replacing the uranium tamper with one madeof lead, for example, the overall explosive force is re-
duced by approximately half but the amount of fallout
is relatively low. The neutron bomb is a hydrogen bomb
with an intentionally thin tamper, allowing as much radi-
ation as possible to escape.
A B C D E
Foam plasma mechanism firing sequence.
1. Warhead before firing; primary (fission bomb) at top, sec-
ondary(fusionfuel) at bottom, allsuspendedin polystyrene
foam.
2. High-explosive fires in primary, compressing plutonium
core into supercriticality and beginning a fission reaction.
3. Fission primary emits X-rays which are scattered along the
inside of the casing, irradiating the polystyrene foam.
4. Polystyrene foam becomes plasma, compressing sec-ondary, and plutonium sparkplug begins to fission.
5. Compressed and heated, lithium-6 deuteride fuel produces
tritium and begins the fusion reaction. The neutron flux
produced causes the U-238 tamper to fission. A fireball
starts to form.
Current technical criticisms of the idea of “foam plasma
pressure” focus on unclassified analysis from similar high
energy physics fields which indicate that the pressure pro-
duced by such a plasma would only be a small multiplier
of the basic photon pressure within the radiation case,
and also that the known foam materials intrinsically have
a very low absorption efficiency of the gamma ray and
X-ray radiation from the primary. Most of the energy
produced would be absorbed by either the walls of the
radiation case and/or the tamper around the secondary.
Analyzing the effects of that absorbed energy led to the
third mechanism: ablation.
3.3 Tamper-pusher ablation
The proposed tamper-pusher ablation mechanism is that
the primary compression mechanism for the thermonu-
clear secondary is that the outer layers of the tamper-pusher, or heavy metal casing around the thermonuclear
fuel, are heated so much by the X-ray flux from the pri-
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6 4 DESIGN VARIATIONS
mary that they ablate away, exploding outwards at such
high speed that the rest of the tamper recoils inwards at
a tremendous velocity, crushing the fusion fuel and the
spark plug.
Ablation mechanism firing sequence.
1. Warhead before firing. The nested spheres at the top are
the fission primary; the cylinders below are the fusion sec-
ondary device.
2. Fission primary’s explosives have detonated and collapsed
the primary’s fissile pit .
3. The primary’s fission reaction has run to completion, and
the primary is now at several million degrees and radiat-
ing gamma and hard X-rays, heating up the inside of the
hohlraum and the shield and secondary’s tamper.
4. The primary’s reaction is over and it has expanded. The
surface of the pusher for the secondary is now so hot that
it is also ablating or expanding away, pushing the rest of
the secondary (tamper, fusion fuel, and fissile spark plug)
inwards. The spark plug starts to fission. Not depicted:
the radiation case is also ablating and expanding outwards (omitted for clarity of diagram).
5. The secondary’s fuel has started the fusion reaction and
shortly will burn up. A fireball starts to form.
Rough calculations for the basic ablation effect are rela-
tively simple: the energy from the primary is distributed
evenly onto all of the surfaces within the outer radiation
case, with the components coming to a thermal equi-
librium, and the effects of that thermal energy are then
analyzed. The energy is mostly deposited within about
one X-ray optical thickness of the tamper/pusher outer
surface, and the temperature of that layer can then becalculated. The velocity at which the surface then ex-
pands outwards is calculated and, from a basic Newtonian
momentum balance, the velocity at which the rest of the
tamper implodes inwards.
Applying the more detailed form of those calculations to
the Ivy Mike device yields vaporized pusher gas expan-
sion velocity of 290 kilometers per second and an implo-
sion velocity of perhaps 400 kilometers per second if 3/4
of the total tamper/pusher mass is ablated off, the most
energy efficient proportion. For the W-80 the gas expan-
sion velocity is roughly 410 kilometers per second and
the implosion velocity 570 kilometers per second. Thepressure due to the ablating material is calculated to be
5.3 billion bar (530 TPa) in the Ivy Mike device and 64
billion bar (6.4 PPa) in the W-80 device.[16]
3.4 Comparing the implosion mechanisms
Comparing the three mechanisms proposed, it can be
seen that:
The calculated ablation pressure is one order of magni-
tude greater than the higher proposed plasma pressures
and nearly two orders of magnitude greater than calcu-
lated radiation pressure. No mechanism to avoid the ab-
sorption of energy into the radiation case wall and the
secondary tamper has been suggested, making ablation
apparently unavoidable. The other mechanisms appear
to be unneeded.
United States Department of Defense official declassifi-
cation reports indicate that foamed plastic materials are
or may be used in radiation case liners, and despite thelow direct plasma pressure they may be of use in de-
laying the ablation until energy has distributed evenly
and a sufficient fraction has reached the secondary’s
tamper/pusher.[17]
Richard Rhodes' book Dark Sun stated that a 1-inch-thick
(25 mm) layer of plastic foam was fixed to the lead liner
of the inside of the Ivy Mike steel casing using copper
nails. Rhodes quotes several designers of that bomb ex-
plaining that the plastic foam layer inside the outer case is
to delay ablation and thus recoil of the outer case: if the
foam were not there, metal would ablate from the inside
of the outer case with a large impulse, causing the casingto recoil outwards rapidly. The purpose of the casing is
to contain the explosion for as long as possible, allowing
as much X-ray ablation of the metallic surface of the sec-
ondary stage as possible, so it compresses the secondary
efficiently, maximizing the fusion yield. Plastic foam has
a low density, so causes a smaller impulse when it ablates
than metal does.[17]
4 Design variations
A number of possible variations to the weapon designhave been proposed:
• Either the tamper or the casing have been proposed
to be made of uranium-235 (highly enriched ura-
nium) in the final fission jacket. The far more ex-
pensive U-235 is also fissionable with fast neutrons
like the standard U-238, but its fission-efficiency is
higher than natural uranium, which is almost en-
tirely U-238. Using a final fissionable jacket of U-
235 would thus be expected to increase the yield of
any Teller-Ulam bomb above a U-238 (depleted ura-
nium) or natural uranium jacket design.
• In some descriptions, additional internal structures
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7
exist to protect the secondary from receiving exces-
sive neutrons from the primary.
• The inside of the casing may or may not be specially
machined to “reflect” the X-rays. X-ray “reflection”
is not like light reflecting off of a mirror, but rather
the reflector material is heated by the X-rays, caus-ing the material itself to emit X-rays, which then
travel to the secondary.
Two special variations exist which will be discussed in a
further section: the cryogenically cooled liquid deuterium
device used for the Ivy Mike test, and the putative design
of the W88 nuclear warhead—a small, MIRVed version
of the Teller–Ulam configuration with a prolate (egg or
watermelon shaped) primary and an elliptical secondary.
Most bombs do not apparently have tertiary “stages”—
that is, third compression stage(s), which are additional
fusion stages compressed by a previous fusion stage (the
fissioning of the last blanket of uranium, which provides
about half the yield in large bombs, does not count as a
“stage” in this terminology).
The U.S. tested three-stage bombs in several explosions
(see Operation Redwing) but is only thought to have
fielded one such tertiary model, i.e., a bomb in which a fis-
sion stage, followed by a fusion stage, finally compresses
yet another fusion stage. This U.S. design was the heavy
but highly efficient (i.e., nuclear weapon yield per unit
bomb weight) 25 Mt B41 nuclear bomb.[18] The Soviet
Union is thought to have used multiple stages (including
more than one tertiary fusion stages) in their 50 megaton
(100 Mt in intended use) Tsar Bomba (however, as with
other bombs, the fissionable jacket could be replaced with
lead in such a bomb, and in this one, for demonstration,
it was). If any hydrogen bombs have been made from
configurations other than those based on the Teller–Ulam
design, the fact of it is not publicly known. (A possible
exception to this is the Soviet early Sloika design).
In essence, the Teller–Ulam configuration relies on at
least two instances of implosion occurring: first, the
conventional (chemical) explosives in the primary would
compress the fissile core, resulting in a fission explosion
many times more powerful than that which chemical ex-
plosives could achieve alone (first stage). Second, the ra-
diation from the fissioning of the primary would be used
to compress and ignite the secondary fusion stage, re-
sulting in a fusion explosion many times more powerful
than the fission explosion alone. This chain of compres-
sion could then be continued with an arbitrary number
of tertiary fusion stages.[19][20] although this is debated
(see more: Arbitrarily large yield debate). Finally, effi-
cient bombs (but not so-called neutron bombs) end with
the fissioning of the final natural uranium tamper, some-
thing which could not normally be achieved without the
neutron flux provided by the fusion reactions in secondaryor tertiary stages. Such designs are suggested to be capa-
ble of being scaled up to an arbitrary large yield (with
apparently as many fusion stages as desired),[19][20] po-
tentially to the level of a "doomsday device.” However,
usually such weapons were not more than a dozen mega-
tons, which was generally considered enough to destroy
even most hardened practical targets (for example, a con-
trol facility such as the Cheyenne Mountain Complex).
Even such large bombs have been replaced by smaller-yield bunker buster type nuclear bombs, see also nuclear
bunker buster.
As discussed above, for destruction of cities and non-
hardened targets, breaking the mass of a single missile
payload down into smaller MIRV bombs, in order to
spread the energy of the explosions into a “pancake” area,
is far more efficient in terms of area-destruction per unit
of bomb energy. This also applies to single bombs deliv-
erable by cruisemissile or other system, such as a bomber,
resulting in most operational warheads in the U.S. pro-
gram having yields of less than 500 kilotons.
5 History
Main article: History of the Teller–Ulam design
5.1 United States
Main articles: Ivy Mike and Operation Castle
The idea of a thermonuclear fusion bomb ignited by a
smaller fission bomb was first proposed by Enrico Fermi
to his colleague Edward Teller in 1941 at the start of
what would become theManhattan Project.[3] Teller spent
most of the Manhattan Project attempting to figure out
how to make the design work, to some degree neglect-
ing his assigned work on the Manhattan Project fission
bomb program. His difficult and devil’s advocate attitude
in discussions led Robert Oppenheimer to sidetrack him
and other “problem” physicists into the super program to
smooth his way.
Stanislaw Ulam, a coworker of Teller, made the first
key conceptual leaps towards a workable fusion design.
Ulam’s two innovations which rendered the fusion bomb
practical were that compression of the thermonuclear fuel
before extreme heating was a practical path towards the
conditions needed for fusion, and the idea of staging or
placing a separate thermonuclear component outside a
fission primary component, and somehow using the pri-
mary to compress the secondary. Teller then realized that
the gamma and X-ray radiation produced in the primary
could transfer enough energy into the secondary to create
a successful implosion and fusion burn, if the whole as-
sembly was wrapped in a hohlraum or radiation case.[3]
Teller and his various proponents and detractors later dis-puted the degree to which Ulam had contributed to the
theories underlying this mechanism. Indeed, shortly be-
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8 5 HISTORY
Operation Castle thermonuclear test, Castle Romeo shot.
fore his death, and in a last-ditch effort to discredit Ulam’s
contributions, Teller claimed that one of his own “gradu-
ate students” had proposed the mechanism.
The “George” shot of Operation Greenhouse of 9 May
1951 tested the basic concept for the first time on a very
small scale. As the first successful (uncontrolled) release
of nuclear fusion energy, which made up a small fractionof the 225kt total yield,[21] it raised expectations to a near
certainty that the concept would work.
On November 1, 1952, the Teller–Ulam configuration
was tested at full scale in the "Ivy Mike" shot at an is-
land in the Enewetak Atoll, with a yield of 10.4 megatons
(over 450 times more powerful than the bomb dropped on
Nagasaki during World War II). The device, dubbed the
Sausage, used an extra-large fission bomb as a “trigger”
and liquid deuterium—kept in its liquid state by 20 short
tons (18 metric tons) of cryogenic equipment—as its fu-
sion fuel, and weighed around 80 short tons (70 metric
tons) altogether.The liquid deuterium fuel of Ivy Mike was impractical
for a deployable weapon, and the next advance was to
use a solid lithium deuteride fusion fuel instead. In 1954
this was tested in the "Castle Bravo" shot (the device was
code-named the Shrimp), which had a yield of 15 mega-
tons (2.5 times higher than expected) and is the largest
U.S. bomb ever tested.
Efforts in the United States soon shifted towards develop-
ing miniaturized Teller–Ulam weapons which could eas-
ily outfit intercontinental ballistic missiles and submarine-
launched ballistic missiles. By 1960, with the W47
warhead[22] deployed on Polaris ballistic missile sub-marines, megaton-class warheads were as small as 18
inches (0.5 m) in diameter and 720 pounds (320 kg) in
weight. It was later found in live testing that the Polaris
warhead did not work reliably and had to be redesigned.
Further innovation in miniaturizing warheads was accom-
plished by the mid-1970s, when versions of the Teller–
Ulam design were created which could fit ten or more
warheads on the end of a small MIRVed missile (see the
section on the W88 below).[7]
5.2 Soviet Union
Main articles: Joe 4 and RDS-37
See also: Soviet atomic bomb project
The first Soviet fusion design, developed by Andrei
Sakharov and Vitaly Ginzburg in 1949 (before the Soviets
had a working fission bomb), was dubbed the Sloika, af-
ter a Russian layer cake, and was not of the Teller–Ulam
configuration. It used alternating layers of fissile mate-
rial and lithium deuteride fusion fuel spiked with tritium
(this was later dubbed Sakharov’s “First Idea”). Though
nuclear fusion might have been technically achievable, it
did not have the scaling property of a “staged” weapon.
Thus, such a design could not produce thermonuclear
weapons whose explosive yields could be made arbitrar-
ily large (unlike U.S. designs at that time). The fusion
layer wrapped around the fission core could only mod-
erately multiply the fission energy (modern Teller–Ulam
designs can multiply it 30-fold). Additionally, the whole
fusion stage had to be imploded by conventional explo-
sives, along with the fission core, multiplying the bulk ofchemical explosives needed substantially.
Their first Sloika design test, RDS-6s, was detonated in
1953 with a yield equivalent to 400 kilotons of TNT (15–
20% from fusion). Attempts to use a Sloika design to
achieve megaton-range results proved unfeasible. After
the U.S. tested the "Ivy Mike" bomb in November 1952,
proving that a multimegaton bomb could be created, the
Soviets searched for an additional design. The “Second
Idea”, as Sakharov referred to it in his memoirs, was a
previous proposal by Ginzburg in November 1948 to use
lithium deuteride in the bomb, which would, in the course
of being bombarded by neutrons, produce tritium andfree deuterium.[23] In late 1953 physicist Viktor Davi-
denko achieved the first breakthrough, that of keeping
the primary and secondary parts of the bombs in separate
pieces (“staging”). The next breakthrough was discovered
and developed by Sakharov and Yakov Zel'dovich, that
of using the X-rays from the fission bomb to compress
the secondary before fusion (“radiation implosion”), in
early 1954. Sakharov’s “Third Idea”, as the Teller–Ulam
design was known in the USSR, was tested in the shot
"RDS-37" in November 1955 with a yield of 1.6 mega-
tons.
The Soviets demonstrated the power of the “staging” con-cept in October 1961, when they detonated the massive
and unwieldy Tsar Bomba, a 50 megaton hydrogen bomb
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5.4 China 9
that derived almost 97% of its energy from fusion. It was
the largest nuclear weapon developed and tested by any
country.
5.3 United Kingdom
Operation Grapple on Christmas Island was the first British hy-
drogen bomb test.
In 1954 work began at Aldermaston to develop the British
fusion bomb, with Sir William Penney in charge of the
project. British knowledge on how to make a thermonu-
clear fusion bomb was rudimentary, and at the time the
United States was not exchanging any nuclear knowledge
because of the Atomic Energy Act of 1946. However,
the British were allowed to observe the American Castle
tests and used sampling aircraft in the mushroom clouds,
providing them with clear, direct evidence of the com-pression produced in the secondary stages by radiation
implosion.
Because of these difficulties, in 1955 British prime min-
ister Anthony Eden agreed to a secret plan, whereby if
the Aldermaston scientists failed or were greatly delayed
in developing the fusion bomb, it would be replaced by
an extremely large fission bomb.
In 1957 the Operation Grapple tests were carried out.
The first test, Green Granite was a prototype fusion
bomb, but failed to produce equivalent yields compared
to the Americans and Soviets, only achieving approxi-
mately 300 kilotons. The second test Orange Herald wasthe modified fission bomb and produced 720 kilotons—
making it the largest fission explosion ever. At the time
almost everyone (including the pilots of the plane that
dropped it) thought that this was a fusion bomb. This
bomb was put into service in 1958. A second prototype
fusion bomb Purple Granite was used in the third test, but
only produced approximately 150 kilotons.
A second set of tests was scheduled, with testing recom-mencing in September 1957. The first test was based on
a "… new simpler design. A two stage thermonuclear
bomb which hada much more powerful trigger”. This test
Grapple X Round C was exploded on November 8 and
yielded approximately 1.8 megatons. On April 28, 1958
a bomb was dropped that yielded 3 megatons—Britain’s
most powerful test. Two final air burst tests on Septem-
ber 2 and September 11, 1958, dropped smaller bombs
that yielded around 1 megaton each.
American observers had been invited to these kinds of
tests. After their successful detonation of a megaton-
range device (and thus demonstrating their practical un-derstanding of the Teller–Ulam design “secret”), the
United States agreed to exchange some of their nuclear
designs with the United Kingdom, leading to the 1958
US–UK Mutual Defence Agreement. Instead of contin-
uing with their own design, the British were given access
to the design of the smaller American Mk 28 warhead
and were able to manufacture copies.
5.4 China
Main article: Test No. 6
The People’s Republic of China detonated its first hydro-
gen bomb on June 17, 1967, 32 months after detonating
its first fission weapon, with a yield of 3.31 Mt. It took
place in the Lop Nor Test Site, in northwest China.[24]
5.5 France
Very little is known about France’s development of the
Teller–Ulam design beyond the fact that France detonated
a 2.6 Mt device in the "Canopus" test in August 1968.
5.6 Other countries
5.6.1 India
Main article: India and weapons of mass destruction
On May 11, 1998, India reportedly detonated a ther-
monuclear bomb in its Operation Shakti tests ("Shakti-
1", specifically).[26] Dr. Samar Mubarakmand asserted
that Shakti-1 was a successful test, but if it was a ther-
monuclear device as claimed, then it failed to producecertain results that were to be expected of a thermonu-
clear device.[26] The yield of India’s hydrogen bomb re-
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10 5 HISTORY
The detonation of Shakti-1 produced a nuclear yield of 45 kt.[25]
mains highly debatable among the Indian science com-
munity and the international scholars.[27] The question of
politicisation and disputes between Indian scientists fur-ther complicated the matter.[28]
Director for the 1998 test site preparations, Dr. K. San-
thanam, reported the yield of the thermonuclear explo-
sion was lower than expected, although his statement
has been disputed by other Indian scientists involved in
the test.[29] Indian sources, using local data and citing a
United States Geological Survey report compiling seismic
data from 125 IRIS stations across the world, argue that
the magnitudes suggested a combined yield of up to 60
kilotonnes, consistent with the Indian announced total
yield of 56 kilotonnes.[30][31] However, several indepen-
dent experts have reported lower yields for the nucleartest and remained skeptical about the claims,[26] and oth-
ers have argued that even the claimed 50 kiloton yield was
low for confirmation of a thermonuclear design.[26][32]
5.6.2 Israel
Main articles: Nuclear weapons and Israel and Vela
Incident
Israel is alleged to possess thermonuclear weapons of the
Teller–Ulam design,[33] but is not known to have testedany nuclear devices, although it is widely speculated that
the Vela Incident of 1979 may have been a joint Israeli-
South African nuclear test.[34][35] It is well established
that American scientist, Edward Teller (father of the hy-
drogen bomb), is said to have advised and guided the Is-
raeli establishment on general nuclear matters for some
twenty years.[36] Between 1964 and 1967, Teller made
six visits to Israel where he lectured at the Tel Aviv Uni-
versity on general topics in theoretical physics.[37] It tookhim a year to convince the CIA about Israel’s capability
and finally in 1976, Carl Duckett of the CIA testified in
the U.S. Congress, after receiving credible information
from an “American scientist” (Edward Teller), on Israel’s
nuclear capability.[35] Sometime in 1990, Teller came to
confirm the speculations in media that it was during his
visits, three decades ago, that he concluded to the CIA
that Israel was in possession of nuclear weapons.[35] Af-
ter he conveyed the matter to the higher level of the U.S.
government, Teller reportedly said: “They [Israel] have
it, and they were clever enough to trust their research and
not to test, they know that to test would get them intotrouble.”[35]
5.6.3 Pakistan
Main article: Pakistan and weapons of mass destruction
According to the scientific data received and published
by PAEC, the Corps of Engineers, and Kahuta Research
Laboratories (KRL), in May 1998, Pakistan carried out
six underground nuclear tests in Chagai Hills and KharanDesert in Balochistan Province (See the code-names of
the tests, Chagai-I and Chagai-II ).[26] None of these
boosted fission devices was the thermonuclear weapon
design, according to KRL and PAEC.[26] In March 2000,
a leading Pakistani theoretical physicist reciprocated Mu-
nir Khan’s statement that both India and Pakistan pos-
sess the scientific capability to produce a hydrogen bomb,
which could be studied and developed “within a time lag
of three to six years.”[33] The scientist maintained that
Pakistan’s policy on hydrogen bombs comes under its
“moral ethics”,[33] and it is a “very dangerous game” since
it would have a destructive impact on the area covering a
radius of about 40–45 miles.[33]
5.6.4 North Korea
Main article: North Korea and weapons of mass destruc-
tion
North Korea’s three nuclear tests (2006, 2009 and 2013)
were relatively low yield and do not appear to have been
of a thermonuclear weapon design. The South Korean
Defense Ministry has speculated that North Korea maybe trying to develop a “hydrogen bomb” and such a device
may be North Korea’s next weapons test.[38][39]
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6.2 The Progressive case 11
6 Public knowledge
The Teller–Ulam design was for many years considered
one of the top nuclear secrets, and even today it is not
discussed in any detail by official publications with ori-
gins “behind the fence” of classification. United States
Department of Energy (DOE) policy has been, and con-
tinues to be, that they do not acknowledge when “leaks”
occur, because doing so would acknowledge the accuracy
of the supposed leaked information.
Photographs of warhead casings, such as this one of the W80
nuclear warhead, allow for some speculation as to the relative
size and shapes of the primaries and secondaries in U.S. ther-
monuclear weapons.
Aside from images of the warhead casing, most informa-
tion in the public domain about this design is relegated to
a few terse statements by the DOE and the work of a few
individual investigators.
6.1 DOE statements
In 1972 the United States government declassified a state-
ment that “The fact that in thermonuclear (TN) weapons,
a fission 'primary' is used to trigger a TN reaction in ther-
monuclear fuel referred to as a 'secondary'", and in 1979
added, “The fact that, in thermonuclear weapons, radia-tion from a fission explosive can be contained and used to
transfer energy to compress and ignite a physically sep-
arate component containing thermonuclear fuel.” To this
latter sentence they specified that "Any elaboration of this
statement will be classified .”[40] The only statement which
may pertain to the spark plug was declassified in 1991:
“Fact that fissile and/or fissionable materials are present
in some secondaries, material unidentified, location un-
specified, use unspecified, and weapons undesignated.” In
1998 the DOE declassified the statement that “The fact
that materials may be present in channels and the term
'channel filler,' with no elaboration”, which may refer tothe polystyrene foam (or an analogous substance).[41]
Whether these statements vindicate some or all of the
models presented above is up for interpretation, and of-
ficial U.S. government releases about the technical de-
tails of nuclear weapons have been purposely equivocat-
ing in the past (see, e.g., Smyth Report). Other informa-
tion, such as the types of fuel used in some of the early
weapons, has been declassified, though of course precise
technical information has not been.
6.2 The Progressive case
Main article: United States v. The Progressive
Most of the current ideas on the workings of the
Teller–Ulam design came into public awareness after the
Department of Energy (DOE) attempted to censor a mag-
azine article by U.S. antiweapons activist Howard Mor-
land in 1979 on the “secret of the hydrogen bomb”. In
1978, Morland had decided that discovering and expos-ing this “last remaining secret” would focus attention onto
the arms race and allow citizens to feel empowered to
question official statements on the importance of nuclear
weapons and nuclear secrecy. Most of Morland’s ideas
about how the weapon worked were compiled from highly
accessible sources—the drawings which most inspired his
approach came from none other than the Encyclopedia
Americana. Morland also interviewed (often informally)
many former Los Alamos scientists (including Teller and
Ulam, though neither gave him any useful information),
and used a variety of interpersonal strategies to encour-
age informative responses from them (i.e., asking ques-tions such as “Do they still use spark plugs?" even if he
was not aware what the latter term specifically referred
to).[42]
Morland eventually concluded that the “secret” was that
the primary and secondary were kept separate and that
radiation pressure from the primary compressed the sec-
ondary before igniting it. When an early draft of the arti-
cle, to be published in The Progressive magazine, was sent
to the DOE after falling into the hands of a professor who
was opposed to Morland’s goal, the DOE requested that
the article not be published, and pressed for a temporary
injunction. The DOE argued that Morland’s informationwas (1) likely derived from classified sources, (2) if not
derived from classified sources, itself counted as “secret”
information under the "born secret" clause of the 1954
Atomic Energy Act, and (3) was dangerous and would
encourage nuclear proliferation.
Morland and his lawyers disagreed on all points, but the
injunction was granted, as the judge in the case felt that
it was safer to grant the injunction and allow Morland,
et al., to appeal, which they did in United States v. The
Progressive (1979).
Through a variety of more complicated circumstances,
the DOE case began to wane as it became clear thatsome of the data they were attempting to claim as “se-
cret” had been published in a students’ encyclopedia a few
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12 7 VARIATIONS
years earlier. After another H-bomb speculator, Chuck
Hansen, had his own ideas about the “secret” (quite dif-
ferent from Morland’s) published in a Wisconsin news-
paper, the DOE claimed that The Progressive case was
moot, dropped its suit, and allowed the magazine to pub-
lish its article, which it did in November 1979. Mor-
land had by then, however, changed his opinion of howthe bomb worked, suggesting that a foam medium (the
polystyrene) rather than radiation pressure was used to
compress the secondary, and that in the secondary there
was a spark plug of fissile material as well. He published
these changes, based in part on the proceedings of the ap-
peals trial, as a short erratum in The Progressive a month
later.[43] In 1981, Morland published a book about his ex-
perience, describing in detail the train of thought which
led him to his conclusions about the “secret”.[42][44]
Morland’s work is interpreted as being at least partially
correct because the DOE had sought to censor it, one of
the few times they violated their usual approach of not ac-knowledging “secret” material which had been released;
however, to what degree it lacks information, or has in-
correct information, is not known with any confidence.
The difficulty that a number of nations had in developing
the Teller–Ulam design (even when they apparently un-
derstood the design, such as with the United Kingdom),
makes it somewhat unlikely that this simple information
alone is what provides the ability to manufacture ther-
monuclear weapons. Nevertheless, the ideas put forward
by Morland in 1979 have been the basis for all the current
speculation on the Teller–Ulam design.
7 Variations
There have been a few variations of the Teller–Ulam de-
sign suggested by sources claiming to have information
from inside of the fence of classification. Whether these
are simply different versions of the Teller–Ulam design,
or should be understood as contradicting the above de-
scriptions, is up for interpretation.
7.1 Richard Rhodes’s “Ivy Mike” device inDark Sun
In his 1995 book Dark Sun: The Making of the Hydro-
gen Bomb, author Richard Rhodes describes in detail the
internal components of the "Ivy Mike" Sausage device,
based on information obtained from extensive interviews
with the scientists and engineers who assembled it. Ac-
cording to Rhodes, the actual mechanism for the com-
pression of the secondary was a combination of the radi-
ation pressure, foam plasma pressure, and tamper-pusher
ablation theories described above; the radiation from the
primary heated the polyethylene foam lining the casing toa plasma, which then re-radiated radiation into the sec-
ondary’s pusher, causing its surface to ablate and driving
In the W88 warhead, the primary (top) and secondary (bottom)
have switched positions, to allow the secondary to be larger than
in the otherwise similar W87.
it inwards, compressing the primary and causing the fu-
sion reaction; the general applicability of this principle is
unclear.[11]
7.2 W88 revelations
In 1999 a reporter for the San Jose Mercury News re-
ported that the U.S. W88 nuclear warhead, a small
MIRVed warhead used on the Trident II SLBM, had a
prolate (egg or watermelon shaped) primary (code-named
Komodo) and a spherical secondary (code-named Cursa)
inside a specially shaped radiation case (known as the
“peanut” for its shape).[45] A story four months later
in The New York Times by William Broad[46] reported
that in 1995, a supposed double agent from the People’s
Republic of China delivered information indicating that
China knew these details about the W88 warhead, sup-posedly through espionage.[47] (This line of investigation
eventually resulted in the abortive trial of Wen Ho Lee.)
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13
In the W87 warhead, the heavier secondary (top) is placed for-
ward of the lighter primary (bottom) to promote aerodynamic
stability during reentry.
If these stories are true, it would explain the reported
higher yield of the W88, 475 kilotons, compared with
only 300 kilotons for the earlier W87 warhead.
The reentry cones for the two warheads are the samesize, 1.75 meters (69 in) long, with a maximum diam-
eter of 55 cm. (22 in).[48] The higher yield of the W88
implies a larger secondary, which produces most of the
yield. Putting the secondary, which is heavier than the
primary, in the wider part of the cone allows it to be
larger, but it also moves thecenter of mass aft, potentially
causing aerodynamic stability problems during reentry.
Dead-weight ballast must be added to the nose to move
the center of mass forward.
To make the primary small enough to fit into the nar-
row part of the cone, its bulky insensitive high explo-
sive charges must be replaced with more compact “non-insensitive” high explosives which are more hazardous to
handle. The higher yield of theW88, which is thelast new
warhead produced by the United States, thus comes at a
price of higher warhead weight and higher workplace haz-
ard. The W88 also contains tritium, which has a half life
of only 12.32 years and must be repeatedly replaced.[49]
8 See also
• Pure fusion weapon
9 References
[1] The misleading term “hydrogen bomb” was already in
wide public use before fission product fallout from the
Castle Bravo test in 1954 revealed the extent to which the
design relies on fission.
[2] From National Public Radio Talk of the Nation, Novem-
ber 8, 2005, Siegfried Hecker of Los Alamos, “the hydro-
gen bomb – that is, a two-stage thermonuclear device, as
we referred to it – is indeed the principal part of the U.S.
arsenal, as it is of the Russian arsenal.”
[3] Teller, Edward; Ulam, Stanislaw (March 9, 1951). “On
Heterocatalytic Detonations I. Hydrodynamic Lenses and
Radiation Mirrors” (PDF). LAMS-1225. Los Alamos
Scientific Laboratory. Retrieved September 26, 2014. on
the Nuclear Non-Proliferation Institute website. This is
the original classified paper by Teller and Ulam propos-
ing staged implosion. This declassified version is heavily
redacted, leaving only a few paragraphs.
[4] Carey Sublette (July 3, 2007). “Nuclear Weapons FAQ
Section 4.4.1.4 The Teller–Ulam Design”. Nuclear
Weapons FAQ . Retrieved 17 July 2011. “So far as is
known all high yield nuclear weapons today (>50 kt or so)
use this design.”
[5] Broad, William J. (23 March 2015). “Hydrogen Bomb
Physicist’s Book Runs Afoul of Energy Department”.
New York Times . Retrieved 20 November 2015.
[6] Greene, Jes (25 March 2015). “A physicist might be in
trouble for what he revealed in his new book about the H
bomb”. Business Insider . Retrieved 20 November 2015.
[7] “Complete List of All U.S. Nuclear Weapons”. 1 October
1997. Retrieved 2006-03-13.
[8] Hansen, Chuck (1988). U.S. nuclear weapons: The secret
history. Arlington, TX: Aerofax. ISBN 0-517-56740-7.
[9] Hansen, Chuck (2007). Swords of Armageddon: U.S.
Nuclear Weapons Development Since 1945 (PDF) (CD-
ROM & download available) (2 ed.). Sunnyvale, Califor-
nia: Chukelea Publications. ISBN 978-0-9791915-0-3.
2,600 pages.
[10] “Figure 5 – Thermonuclear Warhead Components”. Re-
trieved 27 August 2010. A cleaned up version: “BritishH-bomb posted on the Internet by Greenpeace”. Federa-
tion of American Scientists. Retrieved 27 August 2010.
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14 9 REFERENCES
[11] Rhodes, Richard (1995). Dark Sun: The Making of the
Hydrogen Bomb. New York: Simon & Schuster. ISBN
0-684-80400-X.
[12] http://nuclearweaponarchive.org/Usa/Weapons/
W76NeutronTube1200c20.jpg
[13] “Improved Security, Safety & Manufacturability of the
Reliable Replacement Warhead”, NNSA March 2007.
[14] A 1976 drawing which depicts an interstage that absorbs
and re-radiates X-rays. From Howard Morland, “The Ar-
ticle”, Cardozo Law Review, March 2005, p 1374.
[15] [Fogbank] Speculation on Fogbank, Arms Control Wonk
[16] “Nuclear Weapons Frequently Asked Questions 4.4.3.3
The Ablation Process”. 2.04. 20 February 1999. Re-
trieved 2006-03-13.
[17] “Nuclear Weapons Frequently Asked Questions 4.4.4 Im-
plosion Systems”. 2.04. 20 February 1999. Retrieved2006-03-13.
[18] “The B-41 (Mk-41) Bomb – High yield strategic ther-
monuclear bomb”. 21 October 1997. Retrieved 2006-
03-13.
[19] Winterberg, Friedwardt (2010). The Release of Ther-
monuclear Energy by Inertial Confinement: Ways To-
wards Ignition. World Scientific. pp. 192–193. ISBN
9814295914.
[20] Croddy, Eric A.; Wirtz, James J.; Larsen, Jeffrey, Eds.
(2005). Weapons of Mass Destruction: An Encyclope-
dia of Worldwide Policy, Technology, and History . ABC-CLIO, Inc. p. 376. ISBN 1851094903.
[21] The “George” shot, Comprehensive Test Ban Treaty Or-
ganisation website
[22] “Photograph of a W47 warhead” (JPG). Retrieved 2006-
03-13.
[23] Holloway, David (1994). Stalin and the bomb: The Soviet
Union and atomic energy, 1939–1956 . New Haven, CT:
Yale University Press. p. 299. ISBN 0-300-06056-4.
[24] https://www.ctbto.org/specials/testing-times/
17-june-1967-chinas-first-thermonuclear-test
[25] “Forces gung-ho on N-arsenal”. Times of India. Re-
trieved 21 July 2012.
[26] Khan, Kamran (30 May 1998). “Tit-for-Tat: Pakistan
tested 6 nuclear devices in response to Indian’s tests.”. The
News International . Retrieved 10 August 2011. “None
of these explosions were thermonuclear, we are doing re-
search and can do a fusion test if asked, said by Abdul
Qadeer Khan. “These boosted devices are like a half way
stage towards a thermonuclear bomb. They use elements
of the thermonuclear process, and are effectively stronger
Atom bombs”, quoted by Munir Ahmad Khan.
[27] PTI, Press Trust of India (September 25, 2009). “AECex-chief backs Santhanam on Pokhran-II”. The Hindu,
2009. Retrieved 18 January 2013.
[28] Carey Sublette, et. al. “What are the real yield of India’s
Test?". What Are the Real Yields of India’s Test?. Re-
trieved 18 January 2013.
[29] “Former NSA disagrees with scientist, says Pokhran II
successful”. The Times of India. 27 August 2009.
Archived from the original on 30 August 2009. Retrieved
20 November 2015.
[30] India tested H-bomb, says New Scientist
[31] "?". Rediff.com. Retrieved 27 August 2010.
[32] Arms Control Today May 1998, pp. 7–13; Terry C. Wal-
lace, “The May 1998 India and Pakistan Nuclear Tests”
[33] Samdani, Zafar (25 March 2000). “India, Pakistan can
build hydrogen bomb: Scientist”. Dawn News Interviews .
Retrieved 23 December 2012.
[34] Hersh 1991, p. 271.
[35] Cohen, Avner (October 15, 1999). “The Battle over the
NPT: America Learns the Truth”. Israel and the bomb.
(google Book). New York: Columbia University Press.
pp. 297–300. ISBN 978-0231104838.
[36] Karpin, Michael (2005). The Bomb in the Basement . New
York: Simon & Schuster Paperbacks. pp. 289–293.
ISBN 0-7432-6595-5.
[37] Gábor Palló (2000). “The Hungarian Phenomenon in Is-
raeli Science” (PDF). Hungarian Academy of Science 25
(1). Retrieved 11 December 2012.
[38] Kim Kyu-won (February 7, 2013). “North Koreacould bedeveloping a hydrogen bomb”. The Hankyoreh. Retrieved
February 8, 2013.
[39] Kang Seung-woo, Chung Min-uck (February 4, 2013).
“North Korea may detonate H-bomb”. Korea Times. Re-
trieved February 8, 2013.
[40] emphasis in original
[41] Restricted Data Declassification Decisions, 1946 to the
present, Volume 7 . United States Department of Energy.
January 2001.
[42] Morland, Howard (1981). The secret that exploded . New
York: Random House. ISBN 0-394-51297-9.
[43] “The H-Bomb Secret: How we got it and why we’re telling
it”. The Progressive 43 (11). November 1979.
[44] Alexander De Volpi, Jerry Marsh, Ted Postol, and George
Stanford (1981). Born secret: the H-bomb, the Progressive
case and national security. New York: Pergamon Press.
ISBN 0-08-025995-2.
[45] Dan Stober and Ian Hoffman (2001). A convenient spy:
Wen Ho Lee and the politics of nuclear espionage . New
York: Simon & Schuster. ISBN 0-7432-2378-0.
[46] “Spies versus sweat, the debate over China’s nuclear ad-vance”. The New York Times . 7 September 1999. Re-
trieved 2011-04-18.
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15
[47] Christopher Cox, chairman (1999). Report of the United
States House of Representatives Select Committee on U.S.
National Security and Military/Commercial Concerns with
the People’s Republic of China., esp. Ch. 2, “PRC Theft
of U.S. Thermonuclear Warhead Design Information”.
[48] “The W88 Warhead – Intermediate yield strategic SLBM
MIRV warhead”. 1 October 1997. Retrieved 2006-03-
13.
[49] Morland, Howard (February 2003). The holocaust bomb:
A question of time.
9.1 Bibliography
Basic principles
• “Engineering and Design of Nuclear Weapons” from
Carey Sublette’s Nuclear Weapons FAQ.
• Hansen, Chuck, U.S. nuclear weapons: The secret
history (Arlington, TX: Aerofax, 1988). ISBN 0-
517-56740-7
• Hansen, Chuck (2007). Swords of Armaged-
don: U.S. Nuclear Weapons Development Since
1945 (PDF) (CD-ROM & download available) (2
ed.). Sunnyvale, California: Chukelea Publications.
ISBN 978-0-9791915-0-3. 2,600 pages.
• Dalton E. G. Barroso, The physics of nuclear ex-
plosives , in Portuguese. (São Paulo, Brazil: Editora
Livraria da Física, 2009). ISBN 978-85-7861-016-6
History
• DeGroot, Gerard, “The Bomb: A History of Hell
on Earth”, London: Pimlico, 2005. ISBN 0-7126-
7748-8
• Peter Galison and Barton Bernstein, “In any light:
Scientists and the decision to build the Superbomb,
1942–1954” Historical Studies in the Physical and
Biological Sciences Vol. 19, No. 2 (1989): 267–
347.
• German A. Goncharov, “American and Soviet H-
bomb development programmes: historical back-
ground” (trans. A.V. Malyavkin), Physics—Uspekhi
Vol. 39, No. 10 (1996): 1033–1044. Available on-
line (PDF)
• David Holloway, Stalin and the bomb: The Soviet
Union and atomic energy, 1939–1956 (New Haven,
CT: Yale University Press, 1994). ISBN 0-300-
06056-4
• Richard Rhodes, Dark sun: The making of thehydrogen bomb (New York: Simon and Schuster,
1995). ISBN 0-684-80400-X
• S.S. Schweber, In the shadow of the bomb: Bethe,
Oppenheimer, and the moral responsibility of the sci-
entist (Princeton, N.J.: Princeton University Press,
2000). ISBN 0-691-04989-0
• Gary Stix, “Infamy and honor at the Atomic Café:
Edward Teller has no regrets about his contentiouscareer”, Scientific American (October 1999): 42–43.
Analyzing fallout
• Lars-Erik De Geer, “The radioactive signature of
the hydrogen bomb” Science and Global Security
Vol. 2 (1991): 351–363. Available online (PDF)
• Yulii Borisovich Khariton and Yuri Smirnov, The
Khariton version Bulletin of the Atomic Scientists
Vol. 49, No. 4 (May 1993): 20–31.
10 External links
Principles
• “Hydrogen bomb / Fusion weapons” at GlobalSecu-
rity.org (see also links on right)
• “Basic Principles of Staged Radiation Implosion
(Teller–Ulam)" from Carey Sublette’s Nuclear-
WeaponArchive.org.
• “Matter, Energy, and Radiation Hydrodynamics”
from Carey Sublette’s Nuclear Weapons FAQ.
• “Engineering and Designof NuclearWeapons” from
Carey Sublette’s Nuclear Weapons FAQ.
• “Elements of Thermonuclear Weapon Design” from
Carey Sublette’s Nuclear Weapons FAQ.
• Annotated bibliography for nuclear weapons design
from the Alsos Digital Library for Nuclear Issues
History
• PBS: Race for the Superbomb: Interviews and Tran-scripts (with U.S. and USSR bomb designers as well
as historians).
• Howard Morland on how he discovered the “H-
bomb secret” (includes many slides).
• The Progressive November 1979 issue – “The H-
Bomb Secret: How we got it, why we're telling” (en-
tire issue online).
• Annotated bibliography on the hydrogen bomb from
the Alsos Digital Library
• University of Southampton, Mountbatten Centre forInternational Studies, Nuclear History Working Pa-
per No5.
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16 10 EXTERNAL LINKS
• Peter Kuran’s “Trinity and Beyond” – documentary
film on the history of nuclear weapon testing.
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17
11 Text and image sources, contributors, and licenses
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11.2 Images
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• File:Edward_Teller_&_Stanislaw_Ulam_1951_On_Heterocatalytic_Detonations_-_Secret_of_hydrogen_bomb_-_p_1.png
Source: https://upload.wikimedia.org/wikipedia/commons/4/40/Edward_Teller_%26_Stanislaw_Ulam_1951_On_Heterocatalytic_
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data-x-rel='nofollow' class='external text' href='http://www.nuclearnonproliferation.org/LAMS1225.pdf'>Edward Teller, Stanislaw Ulam,
On Heterocatalytic Detonations I: Hydrodynamic Lenses and Radiation Mirrors , Report LAMS-1225, Los Alamos Scientific Laboratory,
March 9, 1951, declassified version, p. 1</a> on Nuclear Nonproliferation Institute website Original artist: Edward Teller and Stanislaw
M. Ulam
• File:Edward_Teller_&_Stanislaw_Ulam_1951_On_Heterocatalytic_Detonations_-_Secret_of_hydrogen_bomb_-_p_3.png
Source: https://upload.wikimedia.org/wikipedia/commons/3/30/Edward_Teller_%26_Stanislaw_Ulam_1951_On_Heterocatalytic_
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data-x-rel='nofollow' class='external text' href='http://www.nuclearnonproliferation.org/LAMS1225.pdf'>Edward Teller, Stanislaw Ulam,
On Heterocatalytic Detonations I: Hydrodynamic Lenses and Radiation Mirrors , Report LAMS-1225, Los Alamos Scientific Laboratory,
March 9, 1951, declassified version, p. 3</a> on Nuclear Nonproliferation Institute website Original artist: Edward Teller and Stanislaw
M. Ulam
• File:Edward_Teller_(1958)-LLNL.jpg Source: https://upload.wikimedia.org/wikipedia/commons/c/cf/Edward_Teller_%281958%
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