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Subject[PATCH] (0/4) Entropy accounting fixes
I've done an analysis of entropy collection and accounting in current
Linux kernels and founds some major weaknesses and bugs. As entropy
accounting is only one part of the security of the random number
device, it's unlikely that these flaws are compromisable, nonetheless
it makes sense to fix them.

- Broken analysis of entropy distribution
- Spoofable delta model
- Interrupt timing independence
- Ignoring time scale of entropy sources
- Confusion of unpredictable and merely complex sources and trusting the
latter
- Broken pool transfers
- Entropy pool can be overrun with untrusted data

Net effect: a typical box will claim to generate 2-5 _orders of magnitude_
more entropy than it actually does.

Note that entropy accounting is mostly useful for things like the
generation of large public key pairs where the number of bits of
entropy in the key is comparable to the size of the PRNG's internal
state. For most purposes, /dev/urandom is still more than strong
enough to make attacking a cipher directly more productive than
attacking the PRNG.

The following patches against 2.5.31 have been tested on x86, but
should compile elsewhere just fine.

I've tried to cover some of the issues in detail below:

Broken analysis of entropy distribution
---------------------------------------
(I know the topic of entropy is rather poorly understood, so here's a couple
useful pieces of background for kernel folks:

Cryptanalytic Attacks on Pseudorandom Number Generators
Kelsey, Schneier, Wagner, Hall
www.counterpane.com/pseudorandom_number.pdf

Cryptographic Randomness from Air Turbulence in Disk Drives
D. Davis, R. Ihaka, P.R. Fenstermacher
http://world.std.com/~dtd/random/forward.ps)

Mathematically defining entropy

For a probability distribution P of samples K, the entropy is:

E = sum (-P(K) * log2 P(K))

For a uniform distribution of n bits of data, the entropy is
n. Anything other than a uniform distribution has less than n bits of
entropy.

Non-Uniform Distribution Of Timing

Unfortunately, our sample source is far from uniform. For starters, each
interrupt has a finite time associated with it - the interrupt latency.
Back to back interrupts will result in samples that are periodically
spaced by a fixed interval.

A priori, we might expect a typical interrupt to be a Poisson
process, resulting in a gamma-like distribution. It would also have
zero probability up to some minimum latency, have a peak at minimum
latency representing the likelihood of back-to-back interrupts, a
smooth hump around the average interrupt rate, and an infinite tail.

Not surprisingly, this distribution has less entropy in it than a
uniform distribution would. Linux takes the approach of assuming the
distribution is "scale invariant" (which is true for exponential
distributions and approximately true for the tails of gamma
distributions) and that the amount of entropy in a sample is in
relation to the number of bits in a given interrupt delta.

Assuming the interrupt actually has a nice gamma-like distribution
(which is unlikely in practice), then this is indeed true. The
trouble is that Linux assumes that if a delta is 13 bits, it contains
12 bits of actual entropy. A moment of thought will reveal that
binary numbers of the form 1xxxx can contain at most 4 bits of
entropy - it's a tautology that all binary numbers start with 1 when
you take off the leading zeros. This is actually a degenerate case of
Benford's Law (http://mathworld.wolfram.com/BenfordsLaw.html), which
governs the distribution of leading digits in scale invariant
distributions.
What we're concerned with is the entropy contained in digits
following the leading 1, which we can derive with a simple extension
of Benford's Law (and some Python):

def entropy(l):
s=0
for pk in l:
if pk: s=s+(-pk*log2(pk))
return s

def benford(digit, place=0, base=10):
if not place:
s=log(1+1.0/digit)
else:
s=0
for k in range(base**(place-1), (base**place)):
s=s+log(1+1.0/(k*base+digit))
print k,s

return s/log(base)

for b in range(3,16):
l=[]
for k in range(1,(2**(b-1))-1):
l.append(benford(k,0,2**(b-1)))
print "%2d %6f" % (b, entropy(l))

Which gives us:

3 1.018740
4 2.314716
5 3.354736
6 4.238990
7 5.032280
8 5.769212
9 6.468756
10 7.141877
11 7.795288
12 8.433345
13 9.059028
14 9.674477
15 10.281286

As it turns out, our 13-bit number has at most 9 bits of entropy, and
as we'll see in a bit, probably significantly less.

All that said, this is easily dealt with by lookup table.

Interrupt Timing Independence
-----------------------------
Linux entropy estimate also wrongly assumes independence of different
interrupt sources. While SMP complicates the matter, this is
generally not the case. Low-priority interrupts must wait on high
priority ones and back to back interrupts on shared lines will
serialize themselves ABABABAB. Further system-wide CLI, cache flushes
and the like will skew -all- the timings and cause them to bunch up
in predictable fashion.

Furthermore, all this is observable from userspace in the same way
that worst-case latency is measured.

To protect against back to back measurements and userspace
observation, we insist that at least one context switch has occurred
since we last sampled before we trust a sample.

Questionable Sources and Time Scales
------------------------------------
Due to the vagarities of computer architecture, things like keyboard
and mouse interrupts occur on their respective scanning or serial
clock edges, and are clocked relatively slowly. Worse, devices like
USB keyboards, mice, and disks tend to share interrupts and probably
line up on USB clock boundaries. Even PCI interrupts have a
granularity on the order of 33MHz (or worse, depending on the
particular adapter), which when timed by a fast processor's 2GHz
clock, make the low six bits of timing measurement predictable.

And as far as I can find, no one's tried to make a good model or
estimate of actual keyboard or mouse entropy. Randomness caused by
disk drive platter turbulence has actually been measured and is on
the order of 100bits/minute and is well correlated on timescales of
seconds - we're likely way overestimating it.

We can deal with this by having each trusted source declare its clock
resolution and removing extra timing resolution bits when we make samples.

Trusting Predictable or Measurable Sources
------------------------------------------
What entropy can be measured from disk timings are very often leaked
by immediately relaying data to web, shell, or X clients. Further,
patterns of drive head movement can be remotely controlled by clients
talking to file and web servers. Thus, while disk timing might be an
attractive source of entropy, it can't be used in a typical server
environment without great caution.

Complexity of analyzing timing sources should not be confused with
unpredictability. Disk caching has no entropy, disk head movement has
entropy only to the extent that it creates turbulence. Network
traffic is potentially completely observable.

(Incidentally, tricks like Matt Blaze's truerand clock drift
technique probably don't work on most PCs these days as the
"realtime" clock source is often derived directly from the
bus/PCI/memory/CPU clock.)

If we're careful, we can still use these timings to seed our RNG, as
long as we don't account them as entropy.

Batching
--------
Samples to be mixed are batched into a 256 element ring
buffer. Because this ring isn't allowed to wrap, it's dangerous to
store untrusted samples as they might flood out trusted ones.

We can allow untrusted data to be safely added to the pool by XORing
new samples in rather than copying and allowing the pool to wrap
around. As non-random data won't be correlated with random data, this
mixing won't destroy any entropy.

Broken Pool Transfers
---------------------
Worst of all, the accounting of entropy transfers between the
primary and secondary pools has been broken for quite some time and
produces thousands of bits of entropy out of thin air.

--
"Love the dolphins," she advised him. "Write by W.A.S.T.E.."
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