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DTSTAMP:20161007T164420Z
UID:4E3F35F9-800B-11E6-96B8-0050568D2FB3
DTSTART;TZID=US/Eastern:20161012T093000
DTEND;TZID=US/Eastern:20161012T170000
DESCRIPTION:The Baltimore Chapter of Electron Devices and Solid-State Circu
 its will be hosting its fifth Fall Colloquium on October 12\, 2016. The th
 eme of this year&#39;s meeting is Quantum Computing. This one-day event featur
 es a variety of experts in multiple aspects of the field: Superconducting 
 Electronics\, Optical Computing\, and Ion Traps. Attendance is open to ind
 ustry\, government\, and academia\, including students. The venue is once 
 again the American Center for Physics (conference room A)\, one mile south
 east of the University of Maryland College Park campus. For location and d
 irections see http://www.acp.org/directions-american-center-physics.\n\nAd
 mission and parking are free\, but registration is required (below). Compl
 imentary lunch will be provided for those who register by October 7. Atten
 dance is limited to 60\; if you are not able to register via this site\, p
 lease contact the chapter secretary papotyraj@ieee.org.\n\nAgenda:\n\n09:0
 0 Registration: Coffee &amp; Donuts\n\n09:45 Opening Remarks\n\n09:55 Dr. Kath
 y-Anne Soderberg\, Air Force Research Laboratory\, Information Directorate
 : &quot;Quantum Networking and Quantum Computing at AFRL&quot;\n\n10:30 Dr. Joel Str
 and\, Northrop Grumman: &quot;Controlling Superconducting Qubits with Josephson
  Junction Logic&quot;\n\n11:05 Dr. Jim Franson\, UMBC: &quot;Nonlinear Properties of
  &#39;Linear&#39; Optical Amplifiers&quot;\n\n11:40 Dr. Jim Freericks\, Georgetown Univ
 ersity: &quot;Measuring Excitation Energies and Green&#39;s Functions in Ion-Trap-B
 ased Quantum Simulations&quot;\n\n12:15 Lunch Break (complimentary lunch provid
 ed for registered attendees)\n\n01:00 Dr. Norbert Linke\, UM Joint Quantum
  Institute: &quot;Quantum Algorithms on a Programmable Ion Trap Quantum Compute
 r&quot;\n\n01:35 Dr. Jiehang Zhang\, UM Joint Quantum Institute: &quot;Non-equilibri
 um Dynamics in an Ion Quantum Simulator&quot;\n\n02:10 Dr. Shuo Sun\, UM Joint 
 Quantum Institute: &quot;Quantum Information Processing with Quantum Dot Spins 
 Coupled to Nanophotonic Cavities&quot;\n\n02:45 Coffee Break\n\n03:00 Dr. Micha
 el Foss-Feig\, Army Research Lab: &quot;Entanglement Growth and Locality in Lon
 g-Range Interacting Quantum Systems&quot;\n\n03:35 Dr. Fredrik Fatemi\, Army Re
 search Lab: &quot;Exciting Modes of Optical Nanofibers&quot;\n\n04:10 Dr. Brian Kirb
 y\, ARL Network Science Division\, &quot;Quantum Network Engineering&quot;\n\n04:45 
 PM - Concluding Remarks\n\n05:00 PM - Adjourn\n\nSpeaker(s): \, \, \, \n\n
 Agenda: \nDr. Joel Strand:  Controlling superconducting qubits requires sh
 aped microwave pulses and\, in most control schemes\, fast flux bias to ac
 hieve the requisite rotations around the Bloch sphere and frequency shifts
  to accomplish a complete set of one and two qubit gates. Sourcing all the
 se control signals at room temperature presents an imposing hardware chall
 enge\, but Reciprocal Quantum Logic (RQL) is a Josephson junction based di
 gital logic that could provide a low power cryogenic source of control sig
 nals. We report on the design\, simulation\, and test of Josephson junctio
 n-based output amplifiers\, microwave switches\, phase shifters\, and bala
 nced modulators operating in the 5-10 GHz range. The devices are controlle
 d by F0-level base-band signals\, operate with no power dissipation on chi
 p\, and have greater than -70 dBm saturation power\, making these devices 
 suitable for control of quantum devices.\n\nDr. James Franson: Optical amp
 lifiers play a crucial role in classical communications\, where they are u
 sed to overcome the loss in optical fibers\, for example. At the quantum l
 evel\, an ideal optical amplifier will introduce an unavoidable amount of 
 noise that must be taken into account in considering their use in applicat
 ions such as quantum communications and quantum sensors. An ideal optical 
 amplifier has long been considered to be a linear device\, but we recently
  showed that entanglement between the signal and the amplifying medium can
  produce large amounts of decoherence that is unrelated to the added noise
 . In fact\, this effect can degrade the performance of an amplifier even w
 hen the added noise is negligibly small. The quantum-mechanical origin of 
 these effects will be discussed and their impact on the amplification of S
 chrodinger cat states will be described.\n\nDr. Jim Freericks: One of the 
 hallmarks of quantum simulation is adiabatic state preparation\, where a s
 ystem starts in the ground state of a trivial Hamiltonian and is slowly ev
 olved to the ground state of a complex Hamiltonian\, which then can be use
 d for further quantum computing or can have its properties analyzed. Since
  most experiments cannot evolve the system over a long-enough time to main
 tain adiabaticity\, and because shortcuts to adiabaticity are difficult to
  achieve\, most quantum simulators create significant diabatic excitations
 . One can directly study these excitations\, by performing spectroscopy to
  extract the excitation energies\, or by using Ramsey-type experiments to 
 extract effective spin-spin Green&#39;s functions. In this talk\, I will descr
 ibe how one performs such spectroscopy and discuss the information contain
 ed in the Green&#39;s functions.\n\nDr. Norbert Linke: Trapped atomic ions pro
 vide pristine &quot;atomic clock&quot; qubits and optical schemes for near-unity sta
 te preparation and measurement. We present a modular quantum computing arc
 hitecture comprised of a chain of Ytterbium ions with individual Raman bea
 m addressing and individual readout [1]. We employ a pulse-shaping scheme 
 [2] to use the transverse modes of motion in the chain to produce entangli
 ng gates between any qubit pair. This creates a fully connected system whi
 ch can be configured to run any sequence of single- and two-qubit gates\, 
 making it in effect an arbitrarily programmable quantum computer. To demon
 strate the universality of this setup\, we present experimental results fr
 om quantum algorithms on five ions.\n\nDr. Jiehang Zhang: We engineer synt
 hetic quantum matter by encoding spins in a linear chain of trapped 171Yb+
  ions. By applying laser-driven spin-dependent transitions\, we generate a
 n effective long-range Ising Hamiltonian\, mediated through the collective
  normal modes of motion. Furthermore\, we apply individual control fields 
 to realize arbitrary state preparation\, as well as programmable random di
 sorder. Such a well-controlled quantum system provides an ideal platform f
 or quantum simulations\, where the classical computation resources require
 d scales exponentially as the system size grows. With these tools\, we pre
 sent some recent studies on intriguing questions regarding to quantum ther
 malization and novel driven phases of matter. We study &quot;prethermalization&quot;
 \, the failure of thermalization due to quasi-conserved quantities. We als
 o present the first observation of a &quot;discrete time-crystal&quot;\, a novel tem
 poral-correlated states which breaks discrete time-translation sysmmetry.\
 n\nDr. Shuo Sun: The spin of a single electron confined in a quantum dot i
 s a promising matter qubit for quantum information processing. This spin s
 ystem possesses microsecond coherence time and allows picosecond timescale
  control using optical pulses. It is also embedded in a host semiconductor
  material that can be directly patterned to form compact integrated nanoph
 otonic devices.\n\nDr. Michael Foss-Feig: For more than a decade\, ultraco
 ld atomic and molecular systems have been exploited to simulate canonical 
 models of strongly correlated materials. However\, the extremely low (ofte
 n sub nano-kelvin) temperatures required to realize the most interesting e
 quilibrium behaviors of such models\, including quantum magnetism and high
 -temperature superconductivity\, have proven extremely difficult to achiev
 e. When these ultracold systems are driven far-from equilibrium\, however\
 , very small temperatures get traded in for very long time-scales\, which 
 enable the observation of dynamic phenomena that were never even envisione
 d in the context of real materials. In this talk\, I will review some rece
 nt experimental and theoretical explorations of non-equilibrium dynamics i
 n ultracold atomic systems\, and will discuss some of the interesting ques
 tions that arise naturally from their remarkable tunability. In particular
 \, I will describe recent efforts to understand the fate of locality --- i
 .e. constraints on the propagation of information/entanglement --- as inte
 ractions become increasingly long-ranged.\n\nDr. Fredrik Fatemi: Optical n
 anofibers (ONFs) - fibers drawn to subwavelength diameters - can have a st
 rong evanescent field that efficiently interacts with surrounding atoms or
  quantum systems. One benefit of ONFs is that they are drawn from standard
  optical fiber that connects well with traditional optical hardware (detec
 tors\, laser diodes\, etc)\, but this requires adiabatic tapering for effi
 cient transmission. In this talk\, I describe the use of higher order opti
 cal modes not only to observe interesting propagation behavior\, but also 
 to measure the ONF radius with 40 picometer sensitivity. I will also descr
 ibe some upcoming experiments we have with trapped cold atoms.\n\nDr. Bria
 n Kirby: The establishment of quantum networks will enable several interes
 ting applications such as secure communication\, distributed quantum compu
 ting\, and enhanced metrology. Quantum networks are comprised of interconn
 ected nodes which are capable of storing\, manipulating\, and transmitting
  entangled quantum states. In this talk we review recent efforts by our gr
 oup at ARL to understand how entanglement can be distributed between these
  nodes in the presence of imperfect channels. First we study the effects o
 f polarization dependent loss\, a common issue in optical fibers\, on enta
 ngled qubit pairs. Further\, we consider the effects of various channel de
 coherence mechanisms on entanglement swapping\, and suggest how networks c
 an be designed to mitigate these. Lastly\, we describe a topology for enta
 nglement-distribution switching networks which is optimized over worst cas
 e loss and the number of switches used.\n\nRoom: Conference Room A\, Bldg:
  American Center for Physics\, One Physics Ellipse\, College Park\, Maryla
 nd\, United States\, 20740
LOCATION:Room: Conference Room A\, Bldg: American Center for Physics\, One 
 Physics Ellipse\, College Park\, Maryland\, United States\, 20740
ORGANIZER:papotyraj@ieee.org
SEQUENCE:13
SUMMARY:Baltimore Colloquium on Quantum Computing
URL;VALUE=URI:https://events.vtools.ieee.org/m/41290
X-ALT-DESC:Description: &lt;br /&gt;&lt;p&gt;The &lt;strong&gt;Baltimore Chapter of Electron 
 Devices and Solid-State Circuits&lt;/strong&gt; will be hosting its fifth &lt;stron
 g&gt;Fall Colloquium&amp;nbsp\;&lt;/strong&gt;on October 12\, 2016.&amp;nbsp\; The theme of
  this year&#39;s meeting is&lt;strong&gt;&amp;nbsp\;Quantum Computing&lt;/strong&gt;.&amp;nbsp\; T
 his one-day event features&amp;nbsp\;a variety of experts in multiple aspects 
 of the field: Superconducting Electronics\, Optical Computing\, and Ion Tr
 aps.&amp;nbsp\; Attendance is open to industry\, government\, and academia\, i
 ncluding students.&amp;nbsp\; The venue is once again the American Center for 
 Physics (conference room A)\, one mile southeast of the University of Mary
 land College Park campus.&amp;nbsp\;&amp;nbsp\;For location and directions see &lt;a 
 href=&quot;http://www.acp.org/directions-american-center-physics&quot;&gt;http://www.ac
 p.org/directions-american-center-physics&lt;/a&gt;.&lt;/p&gt;\n&lt;p&gt;Admission and parkin
 g are free\, but registration is required (below).&amp;nbsp\;&amp;nbsp\;&lt;em&gt;&lt;span 
 style=&quot;color: #800080\;&quot;&gt;Complimentary lunch will be provided for those wh
 o register by October 7&lt;/span&gt;&lt;/em&gt;.&amp;nbsp\; Attendance is limited to 60\; 
 if you are not able to register via this site\, please contact the chapter
  secretary &lt;a href=&quot;mailto:papotyraj@ieee.org&quot;&gt;papotyraj@ieee.org&lt;/a&gt;.&lt;/p&gt;
 \n&lt;p&gt;&amp;nbsp\;&lt;/p&gt;\n&lt;p&gt;&lt;span style=&quot;text-decoration: underline\;&quot;&gt;&lt;strong&gt;Ag
 enda:&lt;/strong&gt;&lt;/span&gt;&lt;/p&gt;\n&lt;p&gt;09:00&amp;nbsp\;Registration: Coffee &amp;amp\; Donu
 ts&lt;/p&gt;\n&lt;p&gt;09:45&amp;nbsp\;Opening Remarks&lt;/p&gt;\n&lt;p&gt;09:55 &lt;strong&gt;Dr. Kathy-Ann
 e Soderberg&lt;/strong&gt;\, Air Force Research Laboratory\, Information Directo
 rate: &quot;&lt;em&gt;Quantum Networking and Quantum Computing at AFRL&lt;/em&gt;&quot;&lt;/p&gt;\n&lt;p&gt;
 10:30 &lt;strong&gt;Dr. Joel Strand&lt;/strong&gt;\, Northrop Grumman: &quot;&lt;em&gt;Controllin
 g Superconducting Qubits with Josephson Junction Logic&lt;/em&gt;&quot;&lt;/p&gt;\n&lt;p&gt;11:05
  &lt;strong&gt;Dr. Jim Franson&lt;/strong&gt;\, UMBC: &lt;em&gt;&quot;Nonlinear Properties of &#39;Li
 near&#39; Optical Amplifiers&quot;&lt;/em&gt;&lt;/p&gt;\n&lt;p&gt;11:40 &lt;strong&gt;Dr. Jim Freericks\,&lt;/
 strong&gt; Georgetown University:&lt;em&gt; &lt;em&gt;&quot;Measuring Excitation Energies and 
 Green&#39;s Functions in Ion-Trap-Based Quantum Simulations&quot;&lt;/em&gt;&lt;/em&gt;&lt;/p&gt;\n&lt;p
 &gt;12:15&amp;nbsp\;Lunch Break &lt;em&gt;(complimentary lunch provided for registered 
 attendees)&amp;nbsp\;&lt;/em&gt;&lt;/p&gt;\n&lt;p&gt;01:00 &lt;strong&gt;Dr. Norbert Linke&lt;/strong&gt;\, 
 UM Joint Quantum Institute: &lt;em&gt;&quot;Quantum Algorithms on a Programmable Ion 
 Trap Quantum Computer&quot;&lt;/em&gt;&lt;/p&gt;\n&lt;p&gt;01:35 &lt;strong&gt;Dr. Jiehang Zhang&lt;/stron
 g&gt;\, UM Joint Quantum Institute: &lt;em&gt;&quot;Non-equilibrium Dynamics in an Ion Q
 uantum Simulator&quot;&lt;/em&gt;&lt;/p&gt;\n&lt;p&gt;02:10 &lt;strong&gt;Dr. Shuo Sun&lt;/strong&gt;\, UM Jo
 int Quantum Institute: &quot;&lt;em&gt;Quantum Information Processing with Quantum Do
 t Spins Coupled to Nanophotonic Cavities&lt;/em&gt;&quot;&lt;/p&gt;\n&lt;p&gt;02:45&amp;nbsp\;Coffee 
 Break&lt;/p&gt;\n&lt;p&gt;03:00&amp;nbsp\;&lt;strong&gt;Dr. Michael Foss-Feig&lt;/strong&gt;\, Army Re
 search Lab: &lt;em&gt;&quot;Entanglement Growth and Locality in Long-Range Interactin
 g Quantum Systems&quot;&lt;/em&gt;&lt;/p&gt;\n&lt;p&gt;03:35 &lt;strong&gt;Dr. Fredrik Fatemi&lt;/strong&gt;\
 , Army Research Lab:&lt;em&gt; &lt;em&gt;&quot;Exciting Modes of Optical Nanofibers&quot;&lt;/em&gt;&lt;/
 em&gt;&lt;/p&gt;\n&lt;p&gt;04:10 &lt;strong&gt;Dr. Brian Kirby\, &lt;/strong&gt;ARL Network Science D
 ivision\, &quot;&lt;em&gt;Quantum Network Engineering&quot;&lt;/em&gt;&lt;/p&gt;\n&lt;p&gt;04:45 PM -&amp;nbsp\;
 Concluding Remarks&lt;/p&gt;\n&lt;p&gt;05:00&amp;nbsp\;PM&amp;nbsp\;- Adjourn&lt;/p&gt;&lt;br /&gt;&lt;br /&gt;A
 genda: &lt;br /&gt;&lt;p&gt;&lt;strong&gt;Dr. Joel Strand: &lt;/strong&gt;&lt;strong&gt;&amp;nbsp\;&lt;/strong&gt;
 Controlling superconducting qubits requires shaped microwave pulses and\, 
 in most control schemes\, fast flux bias to achieve the requisite rotation
 s around the Bloch sphere and frequency shifts to accomplish a complete se
 t of one and two qubit gates.&amp;nbsp\; Sourcing all these control signals at
  room temperature presents an imposing hardware challenge\, but Reciprocal
  Quantum Logic (RQL) is a Josephson junction based digital logic that coul
 d provide a low power cryogenic source of control signals. We report on th
 e design\, simulation\, and test of Josephson junction-based output amplif
 iers\, microwave switches\, phase shifters\, and balanced modulators opera
 ting in the 5-10 GHz range.&amp;nbsp\; The devices are controlled by F&lt;sub&gt;0&lt;/
 sub&gt;-level base-band signals\, operate with no power dissipation on chip\,
  and have greater than -70 dBm saturation power\, making these devices sui
 table for control of quantum devices.&lt;/p&gt;\n&lt;p&gt;&lt;strong&gt;Dr. James Franson&lt;/s
 trong&gt;&lt;strong&gt;:&amp;nbsp\; &lt;/strong&gt;Optical amplifiers play a crucial role in 
 classical communications\, where they are used to overcome the loss in opt
 ical fibers\, for example.&amp;nbsp\; At the quantum level\, an ideal optical 
 amplifier will introduce an unavoidable amount of noise that must be taken
  into account in considering their use in applications such as quantum com
 munications and quantum sensors.&amp;nbsp\; An ideal optical amplifier has lon
 g been considered to be a linear device\, but we recently showed that enta
 nglement between the signal and the amplifying medium can produce large am
 ounts of decoherence that is unrelated to the added noise.&amp;nbsp\; In fact\
 , this effect can degrade the performance of an amplifier even when the ad
 ded noise is negligibly small.&amp;nbsp\; The quantum-mechanical origin of the
 se effects will be discussed and their impact on the amplification of Schr
 odinger cat states will be described.&lt;/p&gt;\n&lt;p&gt;&lt;strong&gt;Dr. Jim Freericks:&amp;n
 bsp\; &lt;/strong&gt;One of the hallmarks of quantum simulation is adiabatic sta
 te preparation\, where a system starts in the ground state of a trivial Ha
 miltonian and is slowly evolved to the ground state of a complex Hamiltoni
 an\, which then can be used for further quantum computing or can have its 
 properties analyzed.&amp;nbsp\; Since most experiments cannot evolve the syste
 m over a long-enough time to maintain adiabaticity\, and because shortcuts
  to adiabaticity are difficult to achieve\, most quantum simulators create
  significant diabatic excitations.&amp;nbsp\; One can directly study these exc
 itations\, by performing spectroscopy to extract the excitation energies\,
  or by using Ramsey-type experiments to extract effective spin-spin Green&#39;
 s functions.&amp;nbsp\; In this talk\, I will describe how one performs such s
 pectroscopy and discuss the information contained in the Green&#39;s functions
 .&lt;/p&gt;\n&lt;p&gt;&lt;strong&gt;Dr. Norbert&amp;nbsp\;Linke:&lt;/strong&gt;&lt;strong&gt;&amp;nbsp\; &lt;/stron
 g&gt;Trapped atomic ions provide pristine &quot;atomic clock&quot; qubits and optical s
 chemes for near-unity state preparation and measurement. &amp;nbsp\;We present
  a modular quantum computing architecture comprised of a chain of Ytterbiu
 m ions with individual Raman beam addressing and individual readout [1].&amp;n
 bsp\; We employ a pulse-shaping scheme [2] to use the transverse modes of 
 motion in the chain to produce entangling gates between any qubit pair.&amp;nb
 sp\; This creates a fully connected system which can be configured to run 
 any sequence of single- and two-qubit gates\, making it in effect an arbit
 rarily programmable quantum computer.&amp;nbsp\; To demonstrate the universali
 ty of this setup\, we present experimental results from quantum algorithms
  on five ions.&lt;/p&gt;\n&lt;p&gt;&lt;strong&gt;Dr. Jiehang Zhang&lt;/strong&gt;&lt;strong&gt;:&amp;nbsp\; 
 &lt;/strong&gt;We engineer synthetic quantum matter by encoding spins in a linea
 r chain of trapped 171Yb+ ions.&amp;nbsp\; By applying laser-driven spin-depen
 dent transitions\, we generate an effective long-range Ising Hamiltonian\,
  mediated through the collective normal modes of motion. &amp;nbsp\;Furthermor
 e\, we apply individual control fields to realize arbitrary state preparat
 ion\, as well as programmable random disorder. &amp;nbsp\;Such a well-controll
 ed quantum system provides an ideal platform for quantum simulations\, whe
 re the classical computation resources required scales exponentially as th
 e system size grows.&amp;nbsp\; With these tools\, we present some recent stud
 ies on intriguing questions regarding to quantum thermalization and novel 
 driven phases of matter.&amp;nbsp\; We study &quot;prethermalization&quot;\, the failure
  of thermalization due to quasi-conserved quantities. &amp;nbsp\;We also prese
 nt the first observation of a &quot;discrete time-crystal&quot;\, a novel temporal-c
 orrelated states which breaks discrete time-translation sysmmetry.&lt;/p&gt;\n&lt;p
 &gt;&lt;strong&gt;Dr. Shuo Sun&lt;/strong&gt;&lt;strong&gt;:&amp;nbsp\; &lt;/strong&gt;The spin of a sing
 le electron confined in a quantum dot is a promising matter qubit for quan
 tum information processing.&amp;nbsp\; This spin system possesses microsecond 
 coherence time and allows picosecond timescale control using optical pulse
 s. &amp;nbsp\;It is also embedded in a host semiconductor material that can be
  directly patterned to form compact integrated nanophotonic devices.&lt;/p&gt;\n
 &lt;p&gt;&lt;strong&gt;Dr. Michael Foss-Feig&lt;/strong&gt;:&amp;nbsp\; For more than a decade\,
  ultracold atomic and molecular systems have been exploited to simulate ca
 nonical models of strongly correlated materials.&amp;nbsp\; However\, the extr
 emely low (often sub nano-kelvin) temperatures required to realize the mos
 t interesting equilibrium behaviors of such models\, including quantum mag
 netism and high-temperature superconductivity\, have proven extremely diff
 icult to achieve.&amp;nbsp\; When these ultracold systems are driven far-from 
 equilibrium\, however\, very small temperatures get traded in for very lon
 g time-scales\, which enable the observation of dynamic phenomena that wer
 e never even envisioned in the context of real materials.&amp;nbsp\; In this t
 alk\, I will review some recent experimental and theoretical explorations 
 of non-equilibrium dynamics in ultracold atomic systems\, and will discuss
  some of the interesting questions that arise naturally from their remarka
 ble tunability.&amp;nbsp\; In particular\, I will describe recent efforts to u
 nderstand the fate of locality --- i.e. constraints on the propagation of 
 information/entanglement --- as interactions become increasingly long-rang
 ed.&lt;/p&gt;\n&lt;p&gt;&lt;strong&gt;Dr. Fredrik Fatemi&lt;/strong&gt;:&amp;nbsp\; Optical nanofibers
  (ONFs) - fibers drawn to subwavelength diameters - can have a strong evan
 escent field that efficiently interacts with surrounding atoms or quantum 
 systems. One benefit of ONFs is that they are drawn from standard optical 
 fiber that connects well with traditional optical hardware (detectors\, la
 ser diodes\, etc)\, but this requires adiabatic tapering for efficient tra
 nsmission.&amp;nbsp\; In this talk\, I describe the use of higher order optica
 l modes not only to observe interesting propagation behavior\, but also to
  measure the ONF radius with 40 picometer sensitivity.&amp;nbsp\; I will also 
 describe some upcoming experiments we have with trapped cold atoms.&lt;/p&gt;\n&lt;
 p&gt;&lt;strong&gt;Dr. Brian Kirby:&amp;nbsp\; &lt;/strong&gt;The establishment of quantum ne
 tworks will enable several interesting applications such as secure communi
 cation\, distributed quantum computing\, and enhanced metrology. &amp;nbsp\;Qu
 antum networks are comprised of interconnected nodes which are capable of 
 storing\, manipulating\, and transmitting entangled quantum states.&amp;nbsp\;
  In this talk we review recent efforts by our group at ARL to understand h
 ow entanglement can be distributed between these nodes in the presence of 
 imperfect channels.&amp;nbsp\; First we study the effects of polarization depe
 ndent loss\, a common issue in optical fibers\, on entangled qubit pairs. 
 Further\, we consider the effects of various channel decoherence mechanism
 s on entanglement swapping\, and suggest how networks can be designed to m
 itigate these.&amp;nbsp\; Lastly\, we describe a topology for entanglement-dis
 tribution switching networks which is optimized over worst case loss and t
 he number of switches used.&lt;/p&gt;
END:VEVENT
END:VCALENDAR

