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<channel>
	<title>QiSci</title>
	<link>http://physics.uq.edu.au/qisci</link>
	<description>The Quantum Information Science Initiative</description>
	<pubDate>Sun, 18 Jan 2009 22:50:49 +0000</pubDate>
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			<item>
		<title>&#8220;Dumb Holes&#8221;</title>
		<link>http://physics.uq.edu.au/qisci/?p=251</link>
		<comments>http://physics.uq.edu.au/qisci/?p=251#comments</comments>
		<pubDate>Wed, 18 Jul 2007 03:01:25 +0000</pubDate>
		<dc:creator>Peter Rohde</dc:creator>
		
		<category><![CDATA[Seminars]]></category>

		<category><![CDATA[General]]></category>

		<guid isPermaLink="false">http://www.qinfo.org/?p=251</guid>
		<description><![CDATA[Date:                   Tuesday 17th July
Who:                   Bill Unruh, University of British Columbia

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			<content:encoded><![CDATA[<p><strong>Date: </strong>                  Tuesday 17th July</p>
<p><strong>Who:</strong>                   Bill Unruh, University of British Columbia</p>
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<p><strong>Seminar type:   </strong>    Research Seminar</p>
<p><strong>Time:     </strong>              1pm</p>
<p><strong>Where:       </strong>          Physics Annexe, CONFFERENCE ROOM, Room 407</p>
<p><strong>Abstract: </strong>        </p>
<p>In this talk Bill Unruh draws analogies between black holes (singularities in space-time) and a fluid-mechanical model of &#8220;dumb holes.&#8221;<br />
It is shown that the horizon of a black-hole is analogous to the point in a fluid system where the background fluid flow exceeds the velocity of sound (and thus sound waves travelling against the flow cannot propagate across this boundary). Unruh comments on the possibility of performing experiments on fluid systems to observe the acoustic analogue of Hawking radiation. This would require measuring power on the order of ~10^-16 Watts in liquid helium, or ~10^-33 Watts in a Bose-Einstein condensate. There is some hope that these miniscule powers might be accessible to experimenters.</p>
]]></content:encoded>
			<wfw:commentRss>http://physics.uq.edu.au/qisci/?feed=rss2&amp;p=251</wfw:commentRss>
		</item>
		<item>
		<title>Monte Carlo simulations of quantum spins in the valence bond basis</title>
		<link>http://physics.uq.edu.au/qisci/?p=239</link>
		<comments>http://physics.uq.edu.au/qisci/?p=239#comments</comments>
		<pubDate>Fri, 08 Jun 2007 03:45:38 +0000</pubDate>
		<dc:creator>Peter Rohde</dc:creator>
		
		<category><![CDATA[Seminars]]></category>

		<category><![CDATA[General]]></category>

		<guid isPermaLink="false">http://www.qinfo.org/?p=239</guid>
		<description><![CDATA[Dear All
Please make a note of Friday&#8217;s research seminar in your diaries.  PLEASE NOTE THAT THE TIME AND VENUE ARE DIFFERENT FROM NORMAL – SEE BELOW!
Date:                   Friday 8th June
Who:        [...]]]></description>
			<content:encoded><![CDATA[<p>Dear All</p>
<p>Please make a note of Friday&#8217;s research seminar in your diaries.  PLEASE NOTE THAT THE TIME AND VENUE ARE DIFFERENT FROM NORMAL – SEE BELOW!</p>
<p><strong>Date: </strong>                  Friday 8th June</p>
<p><strong>Who:</strong>                   Anders Sandvik, Boston University</p>
<p><strong>Seminar type:   </strong>    Research Seminar</p>
<p><strong>Time:     </strong>              2pm</p>
<p><strong>Where:       </strong>          Physics Annexe, CONFFERENCE ROOM, Room 407</p>
<p><strong>Abstract: </strong>        </p>
<p>Traditionally, quantum Monte Carlo simulations of spin hamiltonians have been carried out in the basis of the Sz eigenstates. Here Anders will discuss an alternative technique in which the ground state is projected out from a trial state in the valence bond basis. Thanks to the particular properties of the valence basis, this approach enables calculations of some quantities that are difficult to access with standard methods. In particular, triplet excitations at finite momentum can be studied. Their dispersion relation as well as matrix elements corresponding to the single-magnon peak in the dynamic structure factor can be calculated. Anders will present some results for 1D and 2D Heisenberg antiferromagnets.</p>
]]></content:encoded>
			<wfw:commentRss>http://physics.uq.edu.au/qisci/?feed=rss2&amp;p=239</wfw:commentRss>
		</item>
		<item>
		<title>The Bloch Representation of Quantum States with D &gt; 2</title>
		<link>http://physics.uq.edu.au/qisci/?p=237</link>
		<comments>http://physics.uq.edu.au/qisci/?p=237#comments</comments>
		<pubDate>Tue, 01 May 2007 23:00:27 +0000</pubDate>
		<dc:creator>Peter Rohde</dc:creator>
		
		<category><![CDATA[Seminars]]></category>

		<category><![CDATA[General]]></category>

		<guid isPermaLink="false">http://www.qinfo.org/?p=237</guid>
		<description><![CDATA[&#38;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&#38;amp;amp;amp;amp;amp;amp;amp;amp;gt;Date: &#38;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&#38;amp;amp;amp;amp;amp;amp;amp;amp;gt;      	Friday 4 May
&#38;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&#38;amp;amp;amp;amp;amp;amp;amp;amp;gt;Who:&#38;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&#38;amp;amp;amp;amp;amp;amp;amp;amp;gt;	             Nick Menicucci         	
&#38;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&#38;amp;amp;amp;amp;amp;amp;amp;amp;gt;Seminar type:&#38;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&#38;amp;amp;amp;amp;amp;amp;amp;amp;gt;       Tutorial	
&#38;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&#38;amp;amp;amp;amp;amp;amp;amp;amp;gt;Time:&#38;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&#38;amp;amp;amp;amp;amp;amp;amp;amp;gt;		12pm			
&#38;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&#38;amp;amp;amp;amp;amp;amp;amp;amp;gt;Where:    &#38;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&#38;amp;amp;amp;amp;amp;amp;amp;amp;gt;           [...]]]></description>
			<content:encoded><![CDATA[<p>&amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;Date: &amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;      	Friday 4 May</p>
<p>&amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;Who:&amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;	             Nick Menicucci         	</p>
<p>&amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;Seminar type:&amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;       Tutorial	</p>
<p>&amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;Time:&amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;		12pm			</p>
<p>&amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;Where:    &amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;             Interaction Room	</p>
<p>&amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;Abstract:&amp;amp;amp;amp;amp;amp;amp;amp;amp;lt;/strong&amp;amp;amp;amp;amp;amp;amp;amp;amp;gt;<br />
The Bloch representation of qubits is a particularly convenient way to visualize quantum states and their evolutions.  Every point on the real three-dimensional Bloch sphere is a pure state, all states within the Bloch ball are valid mixed states, and every rotation corresponds to a Hilbert-space unitary.  When generalizing this representation to higher-dimensional systems, none of these properties hold.  For this picture to be useful, then, different intuition is needed.  This tutorial is an introduction to the Bloch representation of quantum states with D &amp;amp;amp;amp;amp;amp;amp;amp;amp;gt; 2 and will emphasize the similarities and differences with the qubit case.<br />
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]]></content:encoded>
			<wfw:commentRss>http://physics.uq.edu.au/qisci/?feed=rss2&amp;p=237</wfw:commentRss>
		</item>
		<item>
		<title>Seminar: The tradeoff between error- and loss-tolerance in quantum error correcting codes</title>
		<link>http://physics.uq.edu.au/qisci/?p=229</link>
		<comments>http://physics.uq.edu.au/qisci/?p=229#comments</comments>
		<pubDate>Fri, 09 Mar 2007 02:56:41 +0000</pubDate>
		<dc:creator>Peter Rohde</dc:creator>
		
		<category><![CDATA[Events]]></category>

		<category><![CDATA[Seminars]]></category>

		<category><![CDATA[General]]></category>

		<guid isPermaLink="false">http://www.qinfo.org/?p=229</guid>
		<description><![CDATA[Date &#038; time: Friday March 9 @ 12pm

Who: Peter Rohde

Seminar type: Research Seminar

Where: Interaction Room

Abstract:
Qubit loss and gate failure are a significant problem in many quantum computing architectures. Most notably this is the case in optical QC where photon loss, inefficient detection, inefficient state preparation, and non-determinsitic gates are a given. To combat these problems [...]]]></description>
			<content:encoded><![CDATA[<p><b>Date &#038; time:</b> Friday March 9 @ 12pm<br />
<br />
<b>Who:</b> Peter Rohde<br />
<br />
<b>Seminar type:</b> Research Seminar<br />
<br />
<b>Where:</b> Interaction Room<br />
<br />
<b>Abstract:</b><br />
Qubit loss and gate failure are a significant problem in many quantum computing architectures. Most notably this is the case in optical QC where photon loss, inefficient detection, inefficient state preparation, and non-determinsitic gates are a given. To combat these problems several authors have proposed schemes for tolerating qubit loss and/or gate failure. These include Nielsen&#8217;s cluster state approach to optical QC, Varnava et al&#8217;s &#8216;horticultural&#8217; approach to loss tolerance, and Ralph et al&#8217;s parity encoding scheme. We demonstrate that while such schemes are very effective at tolerating qubit loss, they have the undesirable side-effect that they magnify the effects of other noise types, namely depolarizing noise. We show that there is a tradeoff relationship between the error- and loss-tolerance of such schemes. This places fundamental limitations on the degree of loss tolerance that is achievable in practise.<br />
<br />
These observations motivate the question &#8216;can we say anything about the tradeoff between loss- and error-tolerance in a general scenario, rather than just for these specific protocols?&#8217;. We examine this question for the general case of non-degenerate codes, by deriving a generalization of the quantum Hamming bound. We derive the Hamming bound to explicitly include separate parameters for loss and depolarizing errors. From this follows an upper bound on the tradeoff between the number of loss and depolarizing errors a non-degenerate code can correct against.<br />
<br />
<b>References:</b></p>
<ul>
<li><i>Upper bounds on the tradeoff between loss and error rates in non-degenerate quantum error correcting codes</i>, Peter Rohde, quant-ph/0605183</li>
<li><i>Error tolerance and tradeoffs in loss- and failure-tolerant quantum computing schemes</i>, Peter Rohde, Timothy Ralph, William Munro, quant-ph/0603130</li>
</ul>
]]></content:encoded>
			<wfw:commentRss>http://physics.uq.edu.au/qisci/?feed=rss2&amp;p=229</wfw:commentRss>
		</item>
		<item>
		<title>The tradeoff between error- and loss-tolerance in quantum error correcting codes</title>
		<link>http://physics.uq.edu.au/qisci/?p=234</link>
		<comments>http://physics.uq.edu.au/qisci/?p=234#comments</comments>
		<pubDate>Tue, 06 Mar 2007 00:18:40 +0000</pubDate>
		<dc:creator>Peter Rohde</dc:creator>
		
		<category><![CDATA[Seminars]]></category>

		<category><![CDATA[General]]></category>

		<guid isPermaLink="false">http://www.qinfo.org/?p=234</guid>
		<description><![CDATA[Date &#038; time: Friday March 9 @ 12pm

Who: Peter Rohde

Seminar type: Research Seminar

Where: Interaction Room

Abstract:
Qubit loss and gate failure are a significant problem in many quantum computing architectures. Most notably this is the case in optical QC where photon loss, inefficient detection, inefficient state preparation, and non-determinsitic gates are a given. To combat these problems [...]]]></description>
			<content:encoded><![CDATA[<p><b>Date &#038; time:</b> Friday March 9 @ 12pm<br />
<br />
<b>Who:</b> Peter Rohde<br />
<br />
<b>Seminar type:</b> Research Seminar<br />
<br />
<b>Where:</b> Interaction Room<br />
<br />
<b>Abstract:</b><br />
Qubit loss and gate failure are a significant problem in many quantum computing architectures. Most notably this is the case in optical QC where photon loss, inefficient detection, inefficient state preparation, and non-determinsitic gates are a given. To combat these problems several authors have proposed schemes for tolerating qubit loss and/or gate failure. These include Nielsen&#8217;s cluster state approach to optical QC, Varnava et al&#8217;s &#8216;horticultural&#8217; approach to loss tolerance, and Ralph et al&#8217;s parity encoding scheme. We demonstrate that while such schemes are very effective at tolerating qubit loss, they have the undesirable side-effect that they magnify the effects of other noise types, namely depolarizing noise. We show that there is a tradeoff relationship between the error- and loss-tolerance of such schemes. This places fundamental limitations on the degree of loss tolerance that is achievable in practise.<br />
<br />
These observations motivate the question &#8216;can we say anything about the tradeoff between loss- and error-tolerance in a general scenario, rather than just for these specific protocols?&#8217;. We examine this question for the general case of non-degenerate codes, by deriving a generalization of the quantum Hamming bound. We derive the Hamming bound to explicitly include separate parameters for loss and depolarizing errors. From this follows an upper bound on the tradeoff between the number of loss and depolarizing errors a non-degenerate code can correct against.<br />
<br />
<b>References:</b></p>
<ul>
<li><i>Upper bounds on the tradeoff between loss and error rates in non-degenerate quantum error correcting codes</i>, Peter Rohde, quant-ph/0605183</li>
<li><i>Error tolerance and tradeoffs in loss- and failure-tolerant quantum computing schemes</i>, Peter Rohde, Timothy Ralph, William Munro, quant-ph/0603130</li>
</ul>
]]></content:encoded>
			<wfw:commentRss>http://physics.uq.edu.au/qisci/?feed=rss2&amp;p=234</wfw:commentRss>
		</item>
		<item>
		<title>A stroboscopic method for observing quantum interference between different coloured photons</title>
		<link>http://physics.uq.edu.au/qisci/?p=232</link>
		<comments>http://physics.uq.edu.au/qisci/?p=232#comments</comments>
		<pubDate>Mon, 22 Jan 2007 23:25:25 +0000</pubDate>
		<dc:creator>Peter Rohde</dc:creator>
		
		<category><![CDATA[Seminars]]></category>

		<category><![CDATA[General]]></category>

		<guid isPermaLink="false">http://www.qinfo.org/?p=232</guid>
		<description><![CDATA[Date:             	THURSDAY 25th January
Who:              	Sean Barrett
Seminar type:     	Research Seminar
Time:		12 Midday
Where:            	Interaction Room
Abstract:
Single photon interference effects [...]]]></description>
			<content:encoded><![CDATA[<p><strong>Date: </strong>            	THURSDAY 25th January</p>
<p><strong>Who:      </strong>        	Sean Barrett</p>
<p><strong>Seminar type: </strong>    	Research Seminar</p>
<p><strong>Time:	</strong>	12 Midday</p>
<p><strong>Where:     </strong>       	Interaction Room</p>
<p><strong>Abstract:</strong><br />
Single photon interference effects are of fundamental interest, and are central to many protocols for quantum information processing (QIP). In particular, effects such as photon bunching and &#8216;which-path&#8217; erasure lie at the heart of many schemes for linear optics quantum computing, and hybrid matter-light QIP. Conventional folklore has that, in order to observe these effects, the photons in question must be identical, in particular that they have the same frequency. Recently, it has been shown that it is possible to observe interference between photons of different frequencies, provided one has photodetectors with sufficiently high temporal resolution. However, this places severe technical constraints on both the sources of these photons, and the detectors.</p>
<p>In this work, we propose a way of observing single photon interference effects between photons of different frequencies, which works even with low resolution detectors. The method is based on carefully controlling the temporal mode shape of the photons, and is roughly analogous to the stroboscopic principle that underlies temporal aliasing, the &#8216;waggon wheel effect&#8217;, and the optical frequency comb that was the subject of the 2005 Nobel prize in physics. The method could allow a much broader range of single photon emitters and matter qubit systems to be used in QIP.</p>
]]></content:encoded>
			<wfw:commentRss>http://physics.uq.edu.au/qisci/?feed=rss2&amp;p=232</wfw:commentRss>
		</item>
		<item>
		<title>Tight informationally complete quantum measurements</title>
		<link>http://physics.uq.edu.au/qisci/?p=231</link>
		<comments>http://physics.uq.edu.au/qisci/?p=231#comments</comments>
		<pubDate>Mon, 08 Jan 2007 01:07:31 +0000</pubDate>
		<dc:creator>Peter Rohde</dc:creator>
		
		<category><![CDATA[General]]></category>

		<guid isPermaLink="false">http://www.qinfo.org/?p=231</guid>
		<description><![CDATA[Date:             	Friday 12th January 2007
Who:              	Andrew Scott
Seminar type:       Research Seminar
Time:			12 Midday
Where:              [...]]]></description>
			<content:encoded><![CDATA[<p><strong>Date: </strong>            	Friday 12th January 2007</p>
<p><strong>Who: </strong>             	Andrew Scott</p>
<p><strong>Seminar type: </strong>      Research Seminar</p>
<p><strong>Time:	</strong>		12 Midday</p>
<p><strong>Where:    </strong>           Interaction Room</p>
<p><strong>Abstract:</strong><br />
We introduce a class of informationally complete positive-operator-valued measures which are, in analogy with a tight frame, &#8220;as close as possible&#8221;<br />
to orthonormal bases for the space of quantum states. These measures are distinguished by an exceptionally simple state-reconstruction formula which allows &#8220;painless&#8221; quantum state tomography. Complete sets of mutually unbiased bases and symmetric informationally complete positive-operator-valued measures are both members of this class, the latter being the unique minimal rank-one members. Recast as ensembles of pure quantum states, the rank-one members are in fact equivalent to weighted 2-designs in complex projective space. These measures are shown to be optimal for (measurement-based) quantum cloning and quantum state tomography.</p>
]]></content:encoded>
			<wfw:commentRss>http://physics.uq.edu.au/qisci/?feed=rss2&amp;p=231</wfw:commentRss>
		</item>
		<item>
		<title>Topology in quantum information</title>
		<link>http://physics.uq.edu.au/qisci/?p=228</link>
		<comments>http://physics.uq.edu.au/qisci/?p=228#comments</comments>
		<pubDate>Sun, 12 Nov 2006 23:27:35 +0000</pubDate>
		<dc:creator>Peter Rohde</dc:creator>
		
		<category><![CDATA[Seminars]]></category>

		<category><![CDATA[General]]></category>

		<guid isPermaLink="false">http://www.qinfo.org/?p=228</guid>
		<description><![CDATA[Date:             	Thursday 16 November
Who:              	Miguel Aguado
Seminar type:     	Tutorial Seminar
Time:		12-1pm
Where:            	Interaction Room
Abstract:
After a review of `classical&#8217; [...]]]></description>
			<content:encoded><![CDATA[<p><strong>Date: </strong>            	Thursday 16 November</p>
<p><strong>Who:    </strong>          	Miguel Aguado</p>
<p><strong>Seminar type: </strong>    	Tutorial Seminar</p>
<p><strong>Time:	</strong>	12-1pm</p>
<p><strong>Where:   </strong>         	Interaction Room</p>
<p><strong>Abstract:</strong><br />
After a review of `classical&#8217; techniques from topology (homotopy, homology, cohomology), some applications to QI will be discussed.  A model of Quantum Computation based on topological ideas (see M. Freedman et al., quant-ph/0001071, 0001108) will be presented.</p>
]]></content:encoded>
			<wfw:commentRss>http://physics.uq.edu.au/qisci/?feed=rss2&amp;p=228</wfw:commentRss>
		</item>
		<item>
		<title>Unconditional security of QKD from causality constrains</title>
		<link>http://physics.uq.edu.au/qisci/?p=227</link>
		<comments>http://physics.uq.edu.au/qisci/?p=227#comments</comments>
		<pubDate>Tue, 07 Nov 2006 01:42:28 +0000</pubDate>
		<dc:creator>Peter Rohde</dc:creator>
		
		<category><![CDATA[Seminars]]></category>

		<category><![CDATA[General]]></category>

		<guid isPermaLink="false">http://www.qinfo.org/?p=227</guid>
		<description><![CDATA[Date:          	Friday 10th November
Who:            	Lluis Masanes
Seminar type:     	Research Seminar
Time:		12 Midday
Where:            	Interaction Room
Abstract:
What is quantum in quantum key distribution (QKD)? All [...]]]></description>
			<content:encoded><![CDATA[<p><strong>Date: </strong>         	Friday 10th November</p>
<p><strong>Who:</strong>            	Lluis Masanes</p>
<p><strong>Seminar type:</strong>     	Research Seminar</p>
<p><strong>Time:</strong>		12 Midday</p>
<p><strong>Where: </strong>           	Interaction Room</p>
<p><strong>Abstract:</strong><br />
What is quantum in quantum key distribution (QKD)? All non-signaling  theories that predict the violation of a Bell inequality share some features with QM: monogamy of correlations, impossibility of perfect cloning, and potentiality for secret communication. This allows for proving the security of some QKD protocols by only assuming the impossibility of arbitrarily fast signaling. In this framework, all the analysis is made at the level of macroscopic events preparations/measurements), hence, Alice and Bob need not trust their devices as long as they produce the desired classical correlations.<br />
Because our assumptions are weaker we give more power to the Eavesdropper, however, it is still possible to get a rate of one secret bit per singlet, as if we where assuming the whole of QM! As a side result, we obtain a classical exponential De Finetti theorem, which makes the i.i.d. assumption no longer necessary in most of classical information theory applications.</p>
]]></content:encoded>
			<wfw:commentRss>http://physics.uq.edu.au/qisci/?feed=rss2&amp;p=227</wfw:commentRss>
		</item>
		<item>
		<title>Quantum Metrology – Part 2</title>
		<link>http://physics.uq.edu.au/qisci/?p=225</link>
		<comments>http://physics.uq.edu.au/qisci/?p=225#comments</comments>
		<pubDate>Fri, 13 Oct 2006 02:17:00 +0000</pubDate>
		<dc:creator>Peter Rohde</dc:creator>
		
		<category><![CDATA[Seminars]]></category>

		<category><![CDATA[General]]></category>

		<guid isPermaLink="false">http://www.qinfo.org/?p=225</guid>
		<description><![CDATA[Date:                   Tuesday 17th October
Who:                    Animesh Datta
Seminar type:        Tutorial Seminar
Time:   [...]]]></description>
			<content:encoded><![CDATA[<p><strong>Date:    </strong>               Tuesday 17th October</p>
<p><strong>Who: </strong>                   Animesh Datta</p>
<p><strong>Seminar type: </strong>       Tutorial Seminar</p>
<p><strong>Time:   </strong>                 4-5pm</p>
<p><strong>Where:   </strong>               Conference Room</p>
<p><strong>Abstract:</strong><br />
Part 2 will deal with the problem of reference frame alignment, which can be seen as an instance of parameter estimation in $\mathrm{SU}(2).$ We will look at some of the methods involved and discuss the results of the analysis. In particular, we will compare the form of the states that achieve the Heisenberg limits in the two problems: clock synchronization and reference frame alignment.</p>
]]></content:encoded>
			<wfw:commentRss>http://physics.uq.edu.au/qisci/?feed=rss2&amp;p=225</wfw:commentRss>
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