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DTSTAMP:20191231T061116Z
UID:F8C71D26-EDAE-463A-B622-763C5B033917
DTSTART;TZID=US/Mountain:20190510T110000
DTEND;TZID=US/Mountain:20190510T121500
DESCRIPTION:Mutually synchronized spin torque nano-oscillators (STNOs) are 
 one of the promising platforms for bioinspired computing and microwave sig
 nal generation [1\,2]. Using STNOs one can achieve 90% recognition rate in
  spoken vowels [3]. However\, in order to do more complex tasks\, larger s
 cale synchronized oscillators are needed\, something that is not easily do
 ne with the STNOs demonstrated so far.\n\nIn my talk\, I will describe a d
 ifferent type of spin current driven device called spin Hall nano-oscillat
 ors (SHNOs)\, which can generate microwave frequencies over a very wide fr
 equency range [4]. The SHNOs are based on 50 – 120 nm wide nano-constric
 tions in Pt(5)/Hf(0.5)/NiFe(3) trilayers (all numbers in nm). When multipl
 e nano-constrictions are fabricated close to each other (300 – 1200 nm s
 eparation) they can mutually synchronize and chains of up to nine nano-con
 strictions have been demonstrated to exhibit complete synchronization [5].
  For the first time\, we can now also synchronize two-dimensional SHNO arr
 ays with as many as 8 x 8 = 64 SHNOs [6]. The mutual synchronization is ob
 served both electrically and using scanning micro-BLS microscopy. Both the
  output power and linewidth of the microwave signal improves substantially
  with increasing number of mutually synchronized SHNOs\, such that quality
  factors of about 170\,000 can be reached. Following the approach of Romer
 a et al [3]\, we also demonstrate neuromorphic computing using a 4 x 4 SHN
 O array with two injected microwave signals as inputs. Given their high op
 erating frequency (~10 GHz)\, easy of fabrication\, and highly robust sync
 hronization properties\, nano-constriction SHNO arrays are likely the most
  promising candidates for neuromorphic computing based on oscillator netwo
 rks.\n\n[1] J. Grollier\, D. Querlioz\, and M. D. Stiles\, Proc. IEEE 104\
 , 2024 (2016)\n\n[2] J. Torrejon et al\, Nature 547\, 428 (2017)\n\n[3] M.
  Romera et al\, Nature 563\, 230–234 (2018)\n\n[4] T. Chen\, R. K. Dumas
 \, A. Eklund\, P. K. Muduli\, A. Houshang\, A. A. Awad\, P. Dürrenfeld\,
  B. G. Malm\, A. Rusu\, and J. Åkerman\, Proc. IEEE 104\, 1919 (2016)\n\n
 [5] A. A. Awad\, P. Dürrenfeld\, A. Houshang\, M. Dvornik\, E. Iacocca\, 
 R. K. Dumas\, and J. Åkerman\, Nature Physics 13\, 292–299 (2017)\n\n[6
 ] M. Zahedinejad\, et al. arXiv:1812.09630 (2018)\n\nCo-sponsored by: UCCS
 \n\nSpeaker(s): Johan Åkerman\, \n\nRoom: A204\, Bldg: Osborne\, 1420 Aus
 tin Bluffs Park\, Colorado Springs\, Colorado\, United States\, 80918
LOCATION:Room: A204\, Bldg: Osborne\, 1420 Austin Bluffs Park\, Colorado Sp
 rings\, Colorado\, United States\, 80918
ORGANIZER:zcelinsk@uccs.edu
SEQUENCE:0
SUMMARY:Two-dimensional mutually synchronized spin Hall nano-oscillator arr
 ays for highly coherent microwave signal generation and neuromorphic compu
 ting.
URL;VALUE=URI:https://events.vtools.ieee.org/m/216643
X-ALT-DESC:Description: &lt;br /&gt;&lt;p&gt;Mutually synchronized spin torque nano-osc
 illators (STNOs) are one of the promising platforms for bioinspired comput
 ing and microwave signal generation [1\,2]. Using STNOs one can achieve 90
 % recognition rate in spoken vowels [3]. However\, in order to do more com
 plex tasks\, larger scale synchronized oscillators are needed\, something 
 that is not easily done with the STNOs demonstrated so far.&lt;/p&gt;\n&lt;p&gt;&amp;nbsp\
 ;&lt;/p&gt;\n&lt;p&gt;In my talk\, I will describe a different type of spin current dr
 iven device called spin Hall nano-oscillators (SHNOs)\, which can generate
  microwave frequencies over a very wide frequency range [4]. The SHNOs are
  based on 50 &amp;ndash\; 120 nm wide nano-constrictions in Pt(5)/Hf(0.5)/NiFe
 (3) trilayers (all numbers in nm).&amp;nbsp\; When multiple nano-constrictions
  are fabricated close to each other (300 &amp;ndash\; 1200 nm separation) they
  can mutually synchronize and chains of up to nine nano-constrictions have
  been demonstrated to exhibit complete synchronization [5]. For the first 
 time\, we can now also synchronize two-dimensional SHNO arrays with as man
 y as 8 x 8 = 64 SHNOs [6]. The mutual synchronization is observed both ele
 ctrically and using scanning micro-BLS microscopy. Both the output power a
 nd linewidth of the microwave signal improves substantially with increasin
 g number of mutually synchronized SHNOs\, such that quality factors of abo
 ut 170\,000 can be reached. Following the approach of Romera et al [3]\, w
 e also demonstrate neuromorphic computing using a 4 x 4 SHNO array with tw
 o injected microwave signals as inputs. Given their high operating frequen
 cy (~10 GHz)\, easy of fabrication\, and highly robust synchronization pro
 perties\, nano-constriction SHNO arrays are likely the most promising cand
 idates for neuromorphic computing based on oscillator networks.&lt;/p&gt;\n&lt;p&gt;&amp;n
 bsp\;&lt;/p&gt;\n&lt;p&gt;[1] &amp;nbsp\; J. Grollier\, D. Querlioz\, and M. D. Stiles\, P
 roc. IEEE &lt;strong&gt;104&lt;/strong&gt;\, 2024 (2016)&lt;/p&gt;\n&lt;p&gt;[2] &amp;nbsp\; J. Torrej
 on et al\, Nature &lt;strong&gt;547&lt;/strong&gt;\, 428 (2017)&lt;/p&gt;\n&lt;p&gt;[3] &amp;nbsp\; M.
  Romera et al\, Nature &lt;strong&gt;563&lt;/strong&gt;\, 230&amp;ndash\;234 (2018)&lt;/p&gt;\n&lt;
 p&gt;[4] &amp;nbsp\; T. Chen\, R. K. Dumas\, A. Eklund\, P. K. Muduli\, A. Housha
 ng\, A. A. Awad\, P. Dürrenfeld\, B. G. Malm\, A. Rusu\, and J. &amp;Aring\;
 kerman\, Proc. IEEE &lt;strong&gt;104&lt;/strong&gt;\, 1919 (2016)&lt;/p&gt;\n&lt;p&gt;[5] &amp;nbsp\;
  A. A. Awad\, P. D&amp;uuml\;rrenfeld\, A. Houshang\, M. Dvornik\, E. Iacocca\
 , R. K. Dumas\, and J. &amp;Aring\;kerman\, Nature Physics &lt;strong&gt;13&lt;/strong&gt;
 \, 292&amp;ndash\;299&amp;nbsp\; (2017)&lt;/p&gt;\n&lt;p&gt;[6] &amp;nbsp\; M. Zahedinejad\, et al
 . arXiv:1812.09630 (2018)&lt;/p&gt;
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