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St. Jude Children's Research Hospital has an outstanding track record of world-class research and innovation, leading to major scientific advances and ground-breaking new inventions in our mission to advance cures, and means of prevention, for pediatric catastrophic diseases through research and treatment. Sometimes, discoveries are made that could be beneficial outside of that mission, and can represent significant opportunities for commercial development.
The Office of Technology Licensing patents inventions with commercial potential and offers them to industry for license. Our goal is to encourage the use of our inventions for the development of products that can be used by researchers and clinicians all over the world, thus benefiting the maximum number of patients. You can explore our technology opportunities for inventions and reagents that are currently available to license.
We are always happy to hear from prospective partners – please contact us if you wish to discuss specific technology interests.
Below is a list of all technologies currently available at St. Jude Children's Research Hospital.
Basic Research Tools
Drug Discovery & Development Tools
Antibodies for Basic Research
Ulk1-/- Ulk2 flox/- hypomorph mice and cell lines (SJ-19-0004)
Research Reagents
Cell Permeabilization Reagent (SJ-07-0007)
CHANGE-seq: a rapid, high-throughput method to define genome-wide activity of CRISPR-Cas genome editors (SJ-18-0041)
Activation of Prodrugs by Carboxylesterase (SJ-98-0001)
Anti-GD2-BB-zeta Chimeric Receptor for Treating GD2+ Malignancies (SJ-13-0035)
Antibodies to Tim4 for use as an Immune Enhancer and Cancer Therapeutic (SJ-18-0006)
Association of Neuraminidase Regulated Exocytosis with Cancer Metastasis (SJ-11-0012)
BCRP/ABCG2 as Stem Cell Marker (SJ-97-0016)
CD33 CAR (SJ-17-0010)
CD7 CAR placed in CD7neg memory cells (SJ-15-0020)
Chimeric gene and protein that can be used to create Optogranules: Light induced stress granules (SJ-18-0010)
Development and Optimization of a Serotype-Independent Method of Adeno-Associated Virus (AAV) Harvest and Purification (SJ-16-0036)
DNA Methylation Profile and Biomarkers for identifying functional T-cells (SJ-17-0002)
DNMT3a knockout CAR T cells with Antigen Specificity (for solid tumors) (SJ-19-0024)
Efficient generation of T-Cell Receptor (TCR) sequences in response to a variety of immune responses (SJ-19-0017)
Erythroid Specific Promoter for Hematopoietic Disorders (SJ-16-0040)
Gene Therapy for Wiskott-Aldrich Syndrome (SJ-19-0012)
Generation of Therapeutic T Cell Receptors for Fibrolamellar Cancer (SJ-19-0046)
HMGA2 in Gene Therapy Vectors (SJ-16-0014)
Hybrid Compounds to treat Gastrointestinal Infections (SJ-14-0019/UTA 14-01)
Immune Cells with DNMT3A Gene Modifications (SJ-16-0009)
Improved Method to Produce Proteins to Treat Lysosomal Storage Disorders (SJ-01-0020)
iNKT Cell Expansion Protocol (SJ-12-0033)
Method for Enhancing Recombinant Antibody Production (SJ-08-0032)
Method for predicting T-cell development stage (and therapy success) (SJ-19-0033)
Minimized Liver Specific Promoter for Improved Gene Expression in Gene Therapy Vectors (SJ-04-0024)
New Method for Differentiating T-cells (SJ-18-0019)
p53 Inhibitory Oligonucloeotides (SJ-09-0015)
Rapid Cloning of T Cell Receptors (SJ-16-0001)
REGNASE-1 Gene Knockout or BATF Overexpression for Improving T-cell Function (SJ-19-0027, SJ-20-0007)
Regulating p53 Translation and Function (SJ-05-0002)
RIPK3 Fusion Protein for Treating Cancer and Autoimmunity (SJ-12-0036)
Safety Test for Gene Therapy Vectors (SJ-15-0027)
A Novel Method for Quantitative Detection of Purines and Their Metabolites (SJ-13-0014)
AML MRD Markers (SJ-18-0011)
Assay for Detecting ALK Inhibitor Resistance Mutations (SJ-09-0042)
Detecting TERT Promoter Methylation for Cancer Diagnosis (SJ-16-0015)
Determining CAR T Cell Effectiveness (SJ-19-0040)
Genotyping Assay to Predict CYP3A5 Phenotype (SJ-01-0005)
Medulloblastoma Subtyping Assay (SJ-10-0020)
Methods for Diagnosing and Treating Learning or Mental Disorders with the SERCA2 Protein and miRNAs that regulate SERCA2 Levels (SJ-10-0003 and SJ-12-0020)
New Markers for Detection of Minimal Residual Disease in Acute Lymphoblastic Leukemia (SJ-11-0025)
XAF-1 Mutations Linked to Cancer Susceptibility (SJ-15-0016)
BET Bromodomain Inhibitors (SJ-16-0032)
Compounds for Treatment of BCR-ABL + Lymphoblastic Leukemias (using an existing malaria drug to overcome resistance) (SJ-11-0042)
CXorf67-PRC2 Interaction and Ependymoma (SJ-17-0030)
DON and small molecule Bcl-2 family antagonists treating glutamine addicted cell lines for Neuroblastomas and Ewing sarcomas (SJ-13-0026)
Improved Human Carboxylesterase for Therapy with CPT-11 (SJ-06-0006)
Method for Improving Learning and Treating Neurological Diseases (SJ-15-0009)
Methods and compositions for the prevention and treatment of hearing loss using CDK2 inhibitors (SJ-14-0028)
New Uses for Chloroquine and Chloroquine Analogs (SJ-02-0008 and SJ-05-0017)
Novel Carboxylesterase Inhibitors (SJ-02-0030)
SARM for Kennedy's Disease (SJ-18-0012)
SPA70 is a potent antagonist of human pregnane X receptor (PXR Antagonists) (SJ-16-0011)
Sudemycins: Synthetic Natural Product Analogs as Anti-Cancer Agents (SJ-08-0026 & SJ-13-0007)
Thalamic microRNA controls the late onset of schizophrenia (SJ-15-0035)
Therapeutic Leads Targeting Influenza Endonuclease (SJ-09-0041)
Transcription Factors for Cochlear Hearing Loss Therapy (SJ-17-0016)
Treating Cochlear Hearing loss with p27Kip1/Atoh1 Combinations (SJ-13-0019)
Use of metabolic drugs to treat influenza infection (SJ-14-0040)
Use of specific retinoid receptor agonists and antagonists as cancer therapies (SJ-14-0011)
Use of Ulk1 modulators to treat thalassemia (SJ-18-0004)
Alternate mTOR Pathway (SJ-09-0021)
ARF and HDM2 interaction domains (SJ-01-0016)
Assay for ATM Kinase Modulation (SJ-02-0008)
BMP Compounds for treating diseases caused by defective or diminished BMP signaling (Medulloblastoma) - (SJ-15-0008)
Caspase 1 inhibition to overcome glucocorticoid resistance (SJ-13-0039)
Cells That Lack p19Ink4d and p27Kip1 Activity/p19Ink4d and p27Kip1 Null Mice (SJ-98-0023)
DCN1 Inhibitors (SJ-16-0002)
Defects in LC3-associated phagocytosis (LAP) associated with Lupus (SJ-16-0025)
Discovery of a fluorescent vinblastine analog with high affinity to the human pregnane X receptor (hPXR) Ligand (SJ-13-0009)
Discovery of a novel inhibitor of constitutive androstane receptor (CAR) that does not activate pregnane X receptor (PXR) (SJ-14-0039)
Hematopoietic progenitor cell lines with myeloid and lymphoid potential (SJ-11-0003)
Identification of Toll-like receptor signaling inhibitors (SJ-18-0008)
Improving HSC Engraftment by Inhibiting GASP Genes (SJ-16-0029)
Interaction of Reelin With Very Low Density Lipoprotein (VLDL) Receptor (SJ-98-0045)
LANDO Pathway Disruption for Alzheimer's Disease (SJ-19-0020)
Modulating Non-Canonical Autophagy (LAP) in Myeloid Cells to Suppress Tumors (SJ-17-0019)
Ozz, A Protein That Regulates Development and Function of Muscle Cells (SJ-99-0010)
Respiratory Cell Isolation and Propagation for Pathogen Study (SJ-18-0028)
SCCRO Peptide Inhibitor (SJ-11-0014)
General Architecture for Defining and Collecting Data (SJ-03-0005)
Multi-slice Myelin Water Imaging (SJ-12-0009)
Phase Cycled Magnetic Resonance Spectroscopic Imaging (SJ-15-0032)
Primary Template-Directed Amplification (PTA) (SJ-18-0003)
ProteinPaint: Web Application for Visualizing Genomic Data (SJ-15-0021)
Statistical Framework for Clinical DNAemia Assays (SJ-18-0039)
System Design and Method for Verifying 3D Dosimetric Imaging (SJ-15-0022)
Attenuated Streptococcus Pneumoniae Strain and Vaccine for Protection Against Pneumococcal Disease (SJ-11-0001)
Avian Influenza Vaccine (SJ-06-0013)
Group B Streptococcus (GBS) Extracellular Matrix Adhesion Proteins (SJ-00-0030)
Improved System for Generating Human Influenza Vaccine in Cell Tissue Culture (SJ-02-0016)
Methods and Composition for Diagnosing and Preventing a Group B Streptococcal Infection (SJ-02-0032)
Modified Influenza Virus for Monitoring and Improving Vaccine Efficiency (SJ-04-0033)
Modified Sendai Virus Vaccine and Imaging Vector (SJ-11-0018)
Reverse Genetics System for Generating RNA Viruses and Vaccines (SJ-00-0006)
Screen to Identify Pneumococcal Proteins that Inhibit Transmission Rather than Invasive Disease (SJ-18-0045)
Synthetic Vaccine and Immunogenic Fusion Proteins for Pneumococcal Infections, and uses (SJ-05-0036, SJ-10-0028, SJ-13-0032)
Universal Influenza Vaccine (SJ-05-0040)
St. Jude Children's Research Hospital discovery aided quest for adult cancer drug
Universal Live Attenuated Pneumonia Vaccine (SJ-11-0001) (Video 2013)
St. Jude's Contribution to Xalkori (Video 2012)
View All Shared Resources
OTL Intellectual Properties Newsletters
The Office of Technology Intellectual Properties Newsletter includes information on the latest technologies licensed and patented by St. Jude Children's Research Hospital as well as contact information for the staff of the Office of Technology Licensing.
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ALL WHO WANDER ARE NOT LOST.
Welcome to Becky's Life: Meandering Down the Long & Winding Road, Wondering What Lies Ahead
** Microfiction Monday **
I decided to give this a try, after seeing it on Janel's Jumble for a few weeks now. Hope I did it correctly! (Hey, Janel, give me a critique, ok??)
Susan at Stony River hosts Microfiction Monday. Susan posts pictures every week and writers take on the challenge to write 140 characters or fewer. (Twitter-sized) stories about the picture.
"Oh dear! What if my husband comes home early and sees his new bride receiving these jars from a delivery service? I told him I could can!"
at May 17, 2010 23 comments:
** Another Manic Monday **
The weekend was a busy and fun one, and this week will be more of the same. It's the week of THE GRADUATION!! Yes, my "baby" graduates from college this week......sniff, sniff..... Where did the years go?
I think I've had about 2 hours of sleep since yesterday. Between Tiger and my new friend, "Arthur", it's getting more and more difficult to get a good night's sleep. Who is Arthur you ask? Why, he's the new pain in my neck....Arthur-Itis! (well....it seemed funny at 3:00 am)
I'll be back later today with news of my May Contest Give-Away.
"Some national parks have long waiting lists for camping reservations. When you have to wait a year to sleep next to a tree, something is wrong." -- George Carlin
at May 17, 2010 6 comments:
CLICK FOR MY FACEBOOK PAGE
Mostly unemployed woman of abundant talents!
Search This Blog For Specific Words
"When you find people who not only tolerate your quirks but celebrate them with glad cries of 'ME, TOO!' be sure to cherish them. Because those weirdos are your tribe."
Nanea Hoffman
MY MEMOIR - Published 2013
CLICK ON COVER FOR MY WEBSITE
Speaking at a Local Library - July 2014
Proud Contributor in 6 Books
Publilshed 2007
Contributed Recipe & WWII True Story
My Publications -Chronological Order
Wash U Center for Humanities (poem about being displaced) April 27, 2020
Wash U Center for the Humanities (poem about distance) April 24, 2020
Wash U Center for the Humanities (poem about a 6 yr old named Opal) April 21, 2020
Rosie's Can Do Cook Booklet (December 2019)
Chicken Soup for the Soul: The Dog Really Did That? (August 2017)
From Pigtails to Chin Hairs: A Memoir & More (Paperback - November 2013, Kindle - March 2014)
Cactus Country III (2013)
Not Your Mother's Book...On Dogs (Dec 2012)
Cuivre River V (October 2010)
Patchwork Path; Treasure Box (November 2010)
Thin Threads; More Real Stories of Life Changing Moments (November 2010)
Vestal Review; Dirty Dozen Micro Fiction (October 2009, January 2010)
Adair County Free Press; (Iowa) Featured weekly columnist March 2008 - April 2010
Tiny Lights - Monthly Search Lights (Sept 2009 - Aug 2014 ~ the finale)
SLU Parks College "Parks Today" Alumni Paper (August 2009)
Beliefnet.com (November 2009)
Chicken Soup for the Soul; Teens Talk Getting In...To College (2008)
Chicken Soup for the Soul; Divorce and Recovery (2008)
Chicken Soup for the Soul; Love Stories (2007)
Chicken Soup for the New Mom's Soul (2007)
Life Happens magazine (2005)
Feast for Body and Soul Cook Book (2002)
St. Charles County Journal; Opinion Columnist (2001-2005)
Some Favorite Quotes
"...IF YOU FOLLOW YOUR BLISS, DOORS WILL OPEN FOR YOU THAT WOULDN'T HAVE OPENED FOR ANYONE ELSE." - Joseph Campbell
"SOMETIMES ON THE WAY TO YOUR DREAM, YOU GET LOST AND FIND A BETTER ONE." - Lisa Hammond
"IT IS POSSIBLE AT ANY AGE TO DISCOVER A LIFELONG DESIRE YOU NEVER KNEW YOU HAD." - Robert Brault
"IT'S NEVER TOO LATE TO BE WHO YOU MIGHT HAVE BEEN." - George Eliot
"WE DID NOT CHANGE AS WE GREW OLDER. WE JUST BECAME MORE CLEARLY OURSELVES." - Lynn Hall
"GO CONFIDENTLY IN THE DIRECTION OF YOUR DREAMS! LIVE THE LIFE YOU HAVE IMAGED." - Henry David Thoreau
Photo Booth!
As Val said, "Good thing your brother was your straight man!"
GREAT WEBSITES FOR WRITERS
PUBLISHING & OTHER FORMS OF INSANITY
CHICKEN SOUP FOR THE SOUL SUBMISSIONS
COMMON ERRORS IN ENGLISH
CREATIVE WRITING NOW
DICTIONARY/Reference
GRAMMARLY DOT COM
IDIOMS - THE FREE DICTIONARY
JENNIE NASH
One of My Mantras
"Follow your bliss.
If you do follow your bliss,
you put yourself on a kind of track
that has been there all the while waiting for you,
and the life you ought to be living
is the one you are living.
When you can see that,
you begin to meet people
who are in the field of your bliss,
and they open the doors to you.
I say, follow your bliss and don't be afraid,
and doors will open
where you didn't know they were going to be.
If you follow your bliss,
doors will open for you that wouldn't have opened for anyone else." -- Joseph Campbell
Book Signing 2014
At Ed & Eva's Shop in Greenfield, Iowa
MEMBER OF, OR SUPPORTER OF, THE FOLLOWING GROUPS
Women's Society of Washington University
St. Louis Writers Guild
Saturday Writers - (president in 2011)
She Writes
Nonfiction Authors Association
Linked In:LinkEds & Writers
Habitat for Humanity; St. Charles County, Mo.
Harlem Children's Zone
Lift for Life Academy
MADD - Mothers Against Drunk Drivers
The Michael J. Fox Foundation
I'm not sure what my dreams are, but I'm anxious to find out. Maybe when I get to that fork in the road, I should take it!
Becky Povich
These writings/blog posts and personal photos may not be used or reproduced in any form without the author's written permission and consent. All protected by copyright law.
OUR BELOVED CHARLIE
Adopted from Shelter 8-year-old, beagle/mix Aug 2016 - Sept 3, 2020
Our beloved Vern
A Shelter Senior Dog. We had him from March 12, 2011 - May 16, 2016
Beloved Tiger Girl
Adopted: shelter 6-month-old puppy: June 1997 - Dec 2010
Our first dog, beloved Rocky, watching over Mark in 1988
Adopted as young puppy: 1983-1997
Blogs I Attempt to Follow!
Unbagging the Cats
Pony House Kitchen: What a Difference a Day Makes
*Terra Garden*
Disraeli TV series, Ian McShane and Bougainvillea
Special Day plans!
6 Agents Actively Seeking Cookbooks, General Nonfiction, Fiction
Obligatory Waste of Time? Or Not? ( #BOTB Results )
Six Questions For . . .
Six Questions for Hatteras Mange, Founder/Editor-in-Chief, Diet Milk Magazine
Writing It Real | Learn from Poet, Essayist & Author Sheila Bender
Another Two New Letters to Those Who Discouraged Us About Our Writing
I Think; Therefore, I Yam
A New Year and a New Life
Drifting through life
Wednesday's Words on a Friday
The Marmelade Gypsy -The Real One
Winter is a Grand Time to Bake!
21 Wits, by Karen
Snow Fairies for Words on Wednesday
Where We Love Is Home
Words for Wednesday 19/1/2022
HOB NOBBERS
CHRISTMAS KEEPS ON GOING
Sioux's Page
Dream Squasher? Or Dream Nurturer?
Sunday Afternoon Tea - Making a Place of Beauty and Peace
Anne R. Allen's Blog
7 Deadly Query Sins: How to Write a Query That Won't End Up in Spam
Respice, Prospice
Daily Spirit
Campo Wind
Elizabeth Seckman, Author
RIP, Friend
The New Robert Brault Reader
That's All, Folks...Farewell and Thanks!
STMcC Presents 'BATTLE OF THE BANDS'
BOTB RESULTS: MARGARITA DAY, 2022 (Or, THE CHAMPS VERSUS JIMMY BUFFETT)
A Touch of Tarragon
Whatever Got Me Through the Night?
Amanda Bretz
Food, Fun, and Frigid Frolicking on a Snowy Pacific Northwest Holiday
Bish Denham
IWSG, News and Onward into the fog...er New Year
#IWSG January 2022 - Regrets, I Have a Few, But Then Again, Too Few to Mention ... (let's get this musical year underway!)
T's Daily Treasures
Stephanie Piro's Cartoon Blog
MERRRRRY Christmas!
Melissa Ann Goodwin, WriterYogini
Life is Beautiful, Life is Hard - The Movie
New Blog Post - Tradition?
Author Jennifer Shirk's Me, My Muse and I
Happy Holidays Sale!
T. Powell Coltrin Writes
December 2021, IWSG
moonbridgebooks
What Makes a Good Food Memoir (besides recipes)
"Southhamsdarling"
UNDER THE TIKI HUT with
Thankfulness is a Warm Turkey
Creative Writing In The Blackberry Patch
The 11th Annual Halloweensie Writing Contest
Memoir Writer's Journey
Mid-Life Adventures: Odyssey of Love by Linda Jamsen: A WOW Blog Tour
Simply Memories and Musings
little wren
Obsessions of a Workaholic
As Deana Carter Would Say, "Did I Shave My Legs for This?"
Adventures in Writing: One Woman's Journey
Victoria Marie Lees [dot] Com is Live
FABBY'S LIVING
A Summer Inspiration Table for Father's Day 2021
Patricia Preston Author Blog
Great Writing Advice!
2020 #Christmas Spirit #ReadingChallenge and #Readathon - Wrap-Up #CSReadathon
A Delightsome Life
Perhaps Today
podso
A Knock at the Door
Chatty Crone
I have a new family - triplets!
Nancy's Notes
TBT Summer and Falling!
NEW BLOG!
Women's Memoirs
Covid-19 Perspectives from Memoir Writers
Green Monkey Tales
Our America, Our Pain, My Voice
Terri Tiffany: Writing Stories You Remember
Catbird Scout
Toby's Last Morning
quirky pickings
Ann's Reading Corner
"3 Month Count Down"
Coming Down the Mountain
Lament of the Empty Nest COVID-19
IWSG and the Polar Murders series
Clara Gillow Clark
LUCKY WINNER of ROOSEVELT BANKS, GOOD-KID-IN-TRAINING
Rose Petals from Heaven
New Instagram Feed
Sue's News, Views 'n Muse
The Best Christmas Carol, a Christmas Story
A geriatric grandmother
A BIG CELEBRATION
All Things Audry
Women Friendships - a Guest Post by Barbara Barth
A Gathering Place
GETTING BACK INTO THE STUDIO
Lydia's Post
Kaisercraft Challenge (#3 Dec)
Musings of an Unapologetic Dreamer
All Along
Bibliophilic Blather
Farewell, Editing for Grammarphobes
Cruisin' with Cricket
In Memory of my sweet Cricket
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a treasured gift
The backing & paper flowers are made with pages from my memoir.
I was a goofy little girl & always kept that sense of humor!
My brother Mike, and me
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redpajama_set_name: RedPajamaCommonCrawl


text:
Washington Monastery celebrates the Solemnity of the Assumption
The Franciscan Monastery of the Holy Land in Washington, D.C., celebrated the Vigil Mass of the Solemnity of the Assumption of Mary on Wednesday evening, August 14. An estimated crowd of nearly 500 people attended the Mass, which was celebrated by the Most Reverend Wilton D. Gregory, recently appointed Archbishop of Washington.
The Archbishop, who was making his first official visit to the Monastery, noted in his homily, that these "wonderful days of summer" are when we "enjoy many of the flowers and much of the produce" planted in the spring. August, he continued "is therefor the perfect time of year to celebrate the Assumption of the Most Blessed Virgin Mary because she is the unique and special harvest of the grace of Jesus' redemptive triumph."
"We honor [Mary] today," he said, "because she is the first to realize the glory that Christ's Resurrection has promised to us all. The Assumption is consequently a celebration of Hope that we too eventually will be raised to the New Life that she now shares perfectly with her Son."
Franciscan Father Larry Dunham, guardian and commissary of the Monastery, thanked the archbishop for his presence, noting that "we hope it will be the first of many such visits."
As a part of the liturgy, a basket of produce from the Monastery's gardens was blessed by the archbishop. The basket represented the more than 14.5 tons of produce raised by the Franciscan Monastery Garden Guild and distributed to area food banks.
The crowd was swelled by incoming students from the Catholic University of America, along with the campus ministry staff of the university. They annually attend this liturgy as part of the opening of the school year.
Music for the liturgy was provided by the choir of St. Anthony of Padua Parish, which is a neighbor of the Monastery in the Brookland area.
Greg Friedman, OFM
Christmas celebrations comes to an end in the Holy Land
The story of the Milk Grotto told in an exhibition
Mons. Rodolfo Cetoloni and his commitment to the Holy Land


text:
Kirchfeld ist der Name folgender Orte:

  Kirchfeld (Gemeinde Ardagger), Ortsteil von Ardagger, Bezirk Amstetten, Niederösterreich
  Kirchfeld (Gemeinde Rosenau), Ortsteil von Rosenau am Hengstpaß, Bezirk Kirchdorf, Oberösterreich
  Kirchfeld (Wörschach), Almweide im Toten Gebirge im Gemeindegebiet von Wörschach, Bezirk Liezen, Österreich

redpajama_set_name: RedPajamaWikipedia


The corporation has decided to install radio frequency meters (RFM) in the border zone.
Plans to replace the two units at the Ropar thermal power plant with an 800 MW thermal units based on supercritical technology. The feasibility study is on.


Seagull Melody formally known as MV REDEMPTION works out of the Gold Coast and is the Party boat when you want to deliver that special event.
In survey for 100 she cruises along at 8- 10 knot on her proven- reliable Caterpillar engines driving though jet propulsion -serviced and maintained, which allows for very shallow draft operating.
Plenty of viewing areas with a top deck that can be used as a dance floor as well as seating. The saloon deck has a dancefloor plus, bar plus two toilets and can be set up with table and chairs for buffet style dining. There is a BBQ facility which is operate aft on the rear platform.
Ranger Flybridge. 2008. 14.2m X 4.2 X 1.3 X 16T Price reduced !!! No expense has been spared to bring this vessel up to a very high standard. A most attractive boat. Powered by twin Yanmar 6LY2-STE 420 hp Turbo diesels, (circa 980 hours) (fitted 2008) an 8 kva Onan genset, plus a large bank of AGM batteries, there is horse power to burn. She has a Polocool 6kw aircon, a full bank of Raymarine electronics, new Muir anchor winch, chain and warp, a Yamaha outboard for the Avon 3.1m RIB, new Victron 80 amp charger, plus all new refrigeration and freezers. Layout is master stateroom, double in saloon plus two singles. A custom after deck has been fitted to extend the cockpit which works very well. This suburb Flybridge cruiser is also fitted with a water maker. Very realistically priced at just $285,000.00 The Owner has just advised us to drop the price to $260,000.00.


text:
\section{Introduction}
Transport through molecular nanodevices\cite{Nitzan2003} has recently been a
subject of intense experimental
 \cite{Reed1997,HPark_2000,JPark_2002,WLiang_2002,Kubatkin_2003,Yu2004,Pasupathy2004,Yu2004b}
 and theoretical
 \cite{Ness2001,Zhang2002,Braig_2003,Flensberg_2003,Mitra_2003,Cornaglia2004,Cornaglia2005a,Chen2004}
 investigation. These systems are not only of
great interest because of their potential for technological
applications but they also pose some interesting an challenging
theoretical problems. They arise because in molecular nanodevices
electron-electron ({\it e--e}) and electron-phonon ({\it e--ph})
interactions are present simultaneously and their interplay may
lead to new physics if their strengths are comparable.

Effects of {\it e--e} interactions in single-molecule devices were
seen through the observation of Coulomb blockade peaks in the
conductance. At these peaks the charge of the molecule changes by
one electron while it stays well defined in the valleys between
them. \cite{Kubatkin_2003}

The Kondo effect \cite{Hewson-book} was also observed in C$_{60}$
single molecules coupled to metallic \cite{Yu2004} and
ferromagnetic electrodes.\cite{Pasupathy2004} It occurs in the
valleys in which the charge of the molecule is close to an odd
integer. Its experimental manifestation is an increase of the
conductance with decreasing temperature and a zero-bias peak in
the differential conductance below a characteristic temperature
scale, the Kondo temperature $T_{\rm K}$.

Furthermore, some features in the I-V characteristics of a
vibrating C$_{60}$ single-molecule transistor were interpreted as
being a manifestation of the effects of the {\it e--ph}
interaction. \cite{HPark_2000}

It was shown in previous work~\cite{Cornaglia2004,Cornaglia2005a}
that the interplay of {\it e--e} and {\it e--ph} interactions has
important effects on the physical properties of the system in the
Kondo regime. There are two different cases characterized by the
strength of the {\it e--ph} coupling. When the latter is weak (in
a sense that will be defined below), the ground state of the
isolated molecule in the odd electron number valleys is a spin
doublet. Then, the conventional Kondo effect appears when the
molecule is coupled to metallic leads. The presence of the {\it
e--ph} interaction results in an increase of the spin fluctuation
energy and of the amplitude of charge fluctuations. In the strong
{\it e--ph} coupling regime, polaronic effects result in an
effective attractive interaction $U_{\rm eff}$ between the
electrons and this leads to qualitatively new physics. If
the charge in the device is close to an odd integer the ground
state of the isolated molecule is a spinless charge doublet. This
is the regime in which the charge Kondo effect develops. It
differs from the conventional Kondo effect in that the low lying
excitations of the system are charge fluctuations whereas spin
fluctuations become increasingly stiff as the {\it e--ph} coupling
increases. The charge Kondo effect enhances the transport through
the molecule and leads to the appearance of a narrow peak in the
conductance as a function of the gate voltage.

In this paper we study the properties of the device in an applied
magnetic field. We found that these are quite different at weak
and strong {\it e--ph} coupling. At weak coupling the system
behaves qualitatively as in the absence of the latter.
\cite{Costi2001} The magnetic field breaks the spin symmetry of
the molecule's ground state and splits the Kondo peak in the
density of states thus suppressing the conductance for fields
$g\mu_BB\gtrsim k_B T_{\rm K}$. At strong coupling, the molecule's
low lying states are spinless and are thus insensitive to the
magnetic field. The Kondo peak is not split by the latter and
there is almost perfect transmission at low temperatures for
fields $B\lesssim B_{\rm crit} = \left|U_{\rm eff}\right|/g\mu_B$.
Furthermore, within this range of field values, the width of the
conductance vs. gate voltage peak increases rapidly with $B$.
Beyond $B_{\rm crit}$ there is level crossing and the conductance
peak splits into two peaks that are strongly spin polarized.

The rest of this paper is organized as follows. In Section
\ref{sec:model} we present the model Hamiltonian and some general
considerations that follow from exact Fermi liquid relationships
at $T=0$. In Section \ref{sec:numerical} we present Numerical
Renormalization Group results for the spin resolved spectral
densities and conductance in the presence of a local magnetic
field at finite temperature and as a function of gate voltage. A
summary and our concluding remarks are presented in Section
\ref{sec:conclusions}.

\section{Model Hamiltonian}\label{sec:model}
We consider a model of a molecule with a single relevant
electronic level coupled to left (L) and right (R) metallic
electrodes and a vibrational mode of frequency $\omega_0$ linearly
coupled to the charge fluctuations of the molecule. The
Hamiltonian of the system is
\begin{equation}
H=H_{M} + H_{E} + H_{M-E}+H_{MF},
\label{hamil}
\end{equation}
where the first three terms describe the isolated molecule, the
electrodes and  their coupling, respectively.  The last term is
the coupling of the spin of the molecule to an external magnetic
field acting only on the molecule. We have
\begin{eqnarray}
H_{M}&=&\varepsilon_d \hat{n}_d + U \hat{n}_{d \uparrow}
\hat{n}_{d \downarrow}-\lambda\;
\left(\hat{n}_d-1 \right)\left(a^{}+a^{\dagger}\right)\nonumber\\
&+&\omega_0a^{\dagger}a^{},\\
H_{E}&=&\sum_{{\bf k},\sigma,\alpha=\{{\rm L,R}\}}
\varepsilon_{\sigma\alpha}({\bf k})\;
c^{\dagger}_{{\bf k} \sigma \alpha} c^{}_{{\bf k} \sigma
\alpha},\\
H_{M-E}&=&\sum_{{\bf k},\sigma,\alpha=\{{\rm L,R}\}}\;V_{{\bf
k}\sigma\alpha}\left(d^{\dagger}_{\sigma}
\;c^{}_{{\bf k}\sigma\alpha} + c^{\dagger}_{{\bf
k}\sigma\alpha}\;d^{}_\sigma \right),\\
H_{MF}&=& g\mu_B B \hat{S}_z^d.
\end{eqnarray}
Here, $\hat{n}_d = \sum_{\sigma} d^{\dagger}_\sigma d^{}_\sigma$
and $\hat{S}_z^d=\frac{1}{2}(d_{\uparrow}^\dagger d_{\uparrow} -
d_{\downarrow}^\dagger d_ {\downarrow})$ are the charge and spin
operators of the molecule, respectively.  The position of the
electronic molecular level relative to the Fermi level of the
electrodes is denoted by $\varepsilon_d$ and $U$ is the Coulomb
repulsion between two electrons that occupy the same molecular
level. Finally, $a^\dag$ is the creation operator of a phonon
of frequency $\omega_0$ and
$\lambda$ is the {\it {\it e--ph}} coupling constant.
We consider for simplicity the case of identical electrodes
with dispersion $\varepsilon_{\rm{R}}({\bf k})
=\varepsilon_{\rm{L}}({\bf k}) =\varepsilon({\bf k})$ and a
${\bf k}$-independent tunnelling matrix element.  We further
assume that the conduction band is symmetric around the chemical
potential and denote its half-width by $D$. In the
following we use units such that $k_B=D=g\mu_B=1$.

The eigenstates of the Hamiltonian $H_M+H_{MF}$ of the isolated
molecule are direct products of electronic states (denoted by a
subscript $e$) and oscillator states. The eigenfunctions  and
their energies can be written explicitly:
\begin{eqnarray}\label{eq:enes}
\begin{array}{ll}
\left |0,m\right> = \tilde{U}^{-}\left |0\right>_e
\left|m\right>\!, & E^0_m=-\frac{\lambda^2}{ \omega_0} +
 m\omega_0 ,\\
\left |\sigma,m\right> = \left |\sigma\right>_e\left|m\right>\!,
 & E^\sigma_m=\varepsilon_d + \sigma B
+ m\omega_0,\\
\left |2,m\right> = \tilde{U}^{+}\left |\uparrow
\downarrow\right>_e\left|m\right>\!, & E^2_m=-{\lambda
^2\over \omega_0} + 2\varepsilon_d + U + m\omega_0,
\end{array}
\end{eqnarray}
where $\tilde{U}^{\pm} =\exp{\left[\pm{\lambda/\omega_0}
\left(a^{\dagger}-a\right)\right]}$, $\left|m\right>$ is the
$m$-th excited state of the harmonic oscillator and $\sigma = \pm
1/2$. The ground state energies of the empty and doubly occupied
electronic states are reduced by the polaronic shift
$\lambda^2/\omega_0$.

At zero field the differences between the occupied and empty
states ${\tilde{E}^\sigma_m} = E^\sigma_m - E^0_m$ and
${\tilde{E}^2_m}- E^0_m$ are ${\tilde{E}^\sigma_m}= \varepsilon_d
+ \lambda^2/\omega_0$ and ${\tilde{E}^2_m}= 2\varepsilon_d + U$,
respectively. The effective interaction between two electrons
occupying the same state is thus ${\tilde{E}^2_m} - 2
{\tilde{E}^\sigma_m} = U- 2\lambda^2/\omega_0 \equiv
U_{\rm eff}$.

The sign of this quantity determines the low energy physics of the
system and its response to an applied field. For positive
$U_{\rm eff}$, the ground state of the isolated molecule is a
spin doublet and the Kondo effect occurs at low temperatures when
the molecule is coupled to the leads.
For negative $U_{\rm eff}$ the ground state of the isolated
molecule is either empty, doubly occupied or a charge doublet. In
the latter case the coupling of the molecule to the leads
generates the charge Kondo effect with an anisotropic Kondo (AK)
exchange coupling.
\cite{Schuttler1988,Cornaglia2004,Cornaglia2005a}

 In this paper we only study the case of
paramagnetic contacts and, therefore, we set $\Gamma_{\sigma
\textsc l}(\omega)=\Gamma_{\sigma \textsc
r}(\omega)\equiv \frac{1}{2}\Gamma(\omega)$, where $\Gamma(\omega)\equiv 2\pi \sum_k
\delta\left(\omega-\varepsilon({\bf k})\right)V_{{\bf k}}^2$.
The spin resolved conductance of the
molecular junction at zero bias
is~\cite{Hershfield1991,Pastawsky1991,Pastawsky1992,Meir1992,Jauho1994}
\begin{equation}
\label{conductance}
G_\sigma={e^2\over h}\ \pi
 \int_{-\infty}^{\infty} d\omega
 \left(-{\partial f(\omega)\over \partial \omega}\right)
 \rho_{d\sigma}({\omega})\Gamma(\omega),
\end{equation}
where $\rho_{d\sigma}(\omega)=-\pi^{-1}{\rm Im}{\mathcal
G}_{d\sigma}(\omega)$, $ {\mathcal
 G}_{d\sigma}(\omega)$ is the retarded electronic Green function of
the molecule in the presence of the leads and $f(\omega)$ is the
Fermi distribution.

At zero temperature, in the wideband limit, the dimensionless
conductance satisfies the Fermi liquid relationship
\begin{equation}
\label{conductance-T0} g\equiv {G \over G_0}=\pi \sum_\sigma
\Gamma\;\rho_{d\sigma}(0)= \sum_\sigma\sin^2\left(\pi
n_{d\sigma}\right),
\end{equation}
where $G_0=e^2/h$ is the quantum of conductance, $n_{d\sigma} =
\langle \hat{n}_{d \sigma}\rangle$, $\Gamma=\Gamma(0)$, and the second equality follows
from Luttinger's theorem \cite{Hewson-book} generalized to the
case in which {\it e--ph} interactions are present.
\cite{Cornaglia2005a}

Consider first the case $\sum_\sigma n_{d\sigma}=1$
corresponding to the electron-hole symmetric situation
$\varepsilon_d = -U/2$. The conductance in zero field is then
$g=2$. In the presence of the applied field $B$ the molecule
acquires a magnetization $m_d=\frac{1}{2}
\left(n_{d\downarrow}-n_{d\uparrow}\right)$ and
Eq.~(\ref{conductance-T0}) becomes
\begin{equation}
 g= \sum_\sigma\sin^2[\pi (1/2 - 2\sigma  m_d)] = 2 \cos^2\left(\pi m_d\right).
\label{eq:luttinger-m}
\end{equation}
In the low field limit we have,
\begin{equation}
 g \approx 2  (1- \pi^2 m_d^2)\approx  2 (1- \pi^2 \chi_d^2  B^2),
\label{g-de-B}
\end{equation}
were $\chi_d=\partial m_d/\partial B$ is the local spin
susceptibility. In the large field limit we have $m_d \to 1/2$ and the
conductance vanishes. The characteristic field beyond which the
conductance is suppressed is $B^{\star} \sim \chi^{-1}_d$.

For $U_{\rm eff}$ large and positive $\chi^{-1}_d \sim T_{\rm K}$
and increases slowly with increasing $\lambda$.
\cite{Cornaglia2004,Cornaglia2005a} Therefore, $B^{\star} \sim
T_{\rm K}$ is small in the limit $U_{\rm eff} \gg \Gamma$. For $B
\gtrsim B^{\star}$ the conductance at $\varepsilon_d\sim -U/2$ is
thus suppressed and $g$ acquires a double-peak structure as a
function of the gate voltage.
 The zero temperature conductance at the positions of the peaks is $g=1$.
\cite{Costi2001}

For $U_{\rm eff}$ large and negative $\chi^{-1}_d \sim
\left|U_{\rm eff}\right|$  and
$B^{\star}$ is thus large.\cite{Cornaglia2004,Cornaglia2005a} In this case, a single conductance peak
with $g=2$ is expected in a broad range of magnetic fields.

In zero field but off electron-hole symmetry, $\varepsilon_d=-U/2
+ \delta \varepsilon_d$, we have:
\begin{equation}
g \approx 2 \;(1- \pi^2 \delta n_d^2/4)\approx 2 \;(1- \pi^2
\chi_c^2 \delta\varepsilon_d^2/4), \label{g-de--e}
\end{equation}
where $\chi_c=-\partial n /\partial \varepsilon_d$ is the charge
susceptibility and $\delta n_d = \sum_\sigma n_{d\sigma} - 1$. The
width $\delta \varepsilon^{\star}_d$ of the conductance peak is
$\sim\!\chi^{-1}_c\!\sim\!T_{{\rm {AK}}}$, the Kondo temperature
of the effective anisotropic Kondo model that is small for very
large $\left|U_{\rm eff}\right|$, $\delta \varepsilon^{\star}_d
\sim \exp\left[- \left(\pi \left|U_{\rm eff}\right|^2/4 \Gamma
\omega_0 \right)\right]$. \cite{Cornaglia2005a}  In the same limit
the field-dependence of $\delta \varepsilon^{\star}_d$ can also be
evaluated analytically (see Eqs.~(\ref{eq:TAK}) and
(\ref{eq:Jakm}) below). We find
\begin{equation}
\frac{\delta \varepsilon^{\star}_d(B)}{\delta
\varepsilon^{\star}_d(0)} \sim \exp\left[ \pi B^2/\left(16 \Gamma
\omega_0 \right)\right]. \label{eq:deltavB}
\end{equation}
The width of the conductance peak thus increases exponentially
with $B^2$ in the strong coupling limit.

\section{Numerical results} \label{sec:numerical}

In this section we present numerical results for the spin resolved
spectral density $\rho_{d\sigma}(\omega)\!=\!- \pi^{-1}{\textrm
{Im}}\;{\mathcal G}_{d\sigma}(\omega)$ and conductance obtained using
the Numerical Renormalization Group method
(NRG) \cite{Wilson1975,Krishnamurthy1980} modified to include {\it {\it e--ph}}
coupling~\cite{Hewson_2002} and to calculate accurately the spectral density
$\rho_{d\sigma}(\omega)$ using the method of
Ref.~[\onlinecite{Hofstetter2000}].

\begin{figure}[tbp]
\includegraphics[width=8.5cm,clip=true]{Densespshift.eps}
\caption{Total and spin-resolved spectral densities at $T=0$ for
$U_{\rm eff}\!>\!0$. Parameters values are
$\varepsilon_d\!=\!-0.04$, $\Gamma\!=\!0.00393$, $U\!=\!0.1$,
$\omega_0\!=\!0.02$, and $U_{\rm eff}\!=\!0.0375$. $T_{\rm
K}\!=\!8\times 10^{-5}$. Full line: total spectral density for
$B=0$. Dotted and dashed lines: spin down and spin up components,
respectively, for $B\!\sim\!T_{\rm K}$. Inset: structure of the
Kondo peak. Full thick and thin lines: total spectral density for
$B\!=\!0$ and $B\!\sim\!T_{\rm K}$, respectively. Dotted and
dashed lines: majority and minority spin components of the
spectral density, respectively.} \label{fig:fig1}
\end{figure}
Figure \ref{fig:fig1} represents the total spectral density in
zero field (full line) and its spin resolved components  (dotted
and dashed lines) in the presence of a small magnetic field
$B\!\sim\!T_{\rm K}$ for a case with $U_{\rm eff} > 0$.
Parameters are $\varepsilon_d\!=\!-0.04$, $\Gamma\!=\!0.00393$,
 $U\!=\!0.1$, $U_{\rm eff}\!=\!0.0375$ and $\omega_0\!=\!0.02$.
The system is off the electron-hole symmetric point and
$\delta\varepsilon_d > 0$, $n_d < 1$. The density of states is
thus asymmetric about the Fermi level,
$\rho_d(\omega)\!\ne\!\rho_d(-\omega)$.
\begin{figure}[tbp]
\includegraphics[width=8.5cm,clip=true]{Cond_mf.eps}
\caption{Zero temperature spectral density in the region of the
Kondo peak and conductance as a function of temperature and
magnetic field at the electron-hole symmetric point. In all cases
$\varepsilon_d\!=\!-0.05$, $\Gamma\!=\!0.01$, and
$\omega_0\!=\!0.05$. (a): Zero temperature spectral density for
$U_{\rm eff}\!=\!0.051$ and three values of the magnetic field.
$T_{\rm K}\!=\!0.004$. (b) Zero temperature spectral density for
$U_{\rm eff}\!=\!-0.044$ and three values of the magnetic field.
$T_{\rm {AK}}\!=\!1.1\times 10^{-4}$. (c) Conductance as a
function of the magnetic field and temperature for $U_{\rm
eff}=0.051$. Temperatures are $T=0$ (top curve) and $T=0.006
\times 2^{-N}, N=0,1,2,\ldots,5$ (from bottom to top). (c)
Conductance as a function of the magnetic field and temperature
for $U_{\rm eff}=-0.044$. Temperatures are as in (b) with
$N=0,1,2,\ldots,9$.} \label{fig:fig2}
\end{figure}
The total spectral function is represented by the full line. We
observe the presence a very narrow Kondo peak near $\omega\!=\!0$
and additional structure on either side of this feature. The Kondo
temperature, determined from the full-width at half maximum of the
central feature, is $T_{\rm K}\!\sim\!8\times 10^{-5}$ for this
set of parameters. The structure on either side of the Kondo peak
are phonon side bands as can be seen by analyzing the pole
structure of ${\cal G}^{\rm at}_{d\sigma}$, the retarded Green
function in the atomic limit ({\it i.e.}, at $\Gamma\!=\!0$).
\cite{Hewson_2002}

The vertical lines in Fig.~\ref{fig:fig1} represent the positions
of the poles of ${\cal G}^{\rm at}_{d\sigma}$ given in Eq.~(15) of
Reference \onlinecite{Hewson_2002}. It can be seen that they are
in fairly good agreement with the positions of the peaks observed
away from the Kondo feature in Fig.~\ref{fig:fig1}.

The presence of a field $B\!\sim\!T_{\rm K}$ has drastic
effects on the spin resolved spectral spectral function. Due to
the high magnetic susceptibility of the molecule ($\propto
1/T_{\rm K}$) the latter acquires  a large magnetization. Most
of the electron density is composed of majority spins (down spins)
and the population of the minority spins (up spins) is small. The
spectral function of the majority spins (represented by dotted
lines) is thus large for $\omega\!<\!0$ whereas that of the
minority spins (represented by dashed lines) is large for
$\omega\!>\!0$.

The inset to the figure shows in detail the effect of the magnetic
field on the Kondo peak. The thick and thin full lines represent
the total spectral function in the central region in zero field
and  for $B\!\sim\!T_{\rm K}$, respectively. It can be seen that
the Kondo peak splits and its amplitude is reduced anticipating
the suppression of the Kondo effect at higher fields. The dotted
and dashed lines represent the spin down and spin up components of
$\rho_d(\omega)$, respectively. It is seen that position of the
two Kondo peaks shift in opposite directions by an amount $\sim
\pm B$.  \cite{Costi2001}

Figure \ref{fig:fig2} displays the spin resolved spectral density
at $T\!=\!0$ for three values of the magnetic field (a,b), and the
conductance as a function of  magnetic field and temperature (c,d)
at the electron-hole symmetric point. The parameters are
$\Gamma\!=\!0.01$, $U\!=\!0.1$, and $\omega_0\!=\!0.05$. We only
show the minority-spin spectral density $\rho_{d\uparrow}$ since
electron-hole symmetry and spin reversal invariance lead to the
relationship
$\rho_{d\downarrow}(\omega)=\rho_{d\uparrow}(-\omega)$.

It can be seen that the Kondo peak behaves differently in a
magnetic field in the cases shown in Fig.~{\ref{fig:fig2}}(a)
($U_{\rm eff}\!=\!0.051\!>0$) and Fig.~{\ref{fig:fig2}}(b)
($U_{\rm eff}\!=\!-0.044\!<\!0$). Whereas in the former case the
Kondo peak shifts and its hight decreases upon applying a small
magnetic field, in the latter case, for fields $B\!\lesssim
\left|U_{\rm eff}\right|$, its position and height remain
unchanged. Note that the shape of the peak is asymmetric and its
width increases sharply upon applying the field. The spectral
asymmetry is due to the decrease of the density of minority spins
in the presence of the field as discussed above. The
field-dependence of the width of the Kondo peak will be discussed
below.

For even larger fields, $B\!>\left|U_{\rm eff}\right|$,
there is a level crossing and the charge doublet is no longer the
 ground state of the isolated molecule. The charge Kondo effect can not
take place and the associated peak in the density of states
disappears.
\begin{figure}[tbp]
\includegraphics[width=8.5cm,clip=true]{Gcond_e_cMF.eps}
\caption{Zero temperature conductance $G$ versus gate voltage
 $\varepsilon_d$ for different values of the magnetic field B in the strong {\it
e--ph} coupling regime (a-d). Solid lines: total conductance.
Dashed and dotted lines: majority (down) and minority (up) spins, respectively.
Other parameters as in Fig \ref{fig:fig2}(b).} \label{fig:fig3}
\end{figure}

The dependence of the conductance on field and temperature for the
cases of positive and negative $U_{\rm eff}$ is shown in
Figs.~\ref{fig:fig2}(c) and \ref{fig:fig2}(d), respectively.

For positive $U_{\rm eff}$, the field-induced suppression of
spectral weight at the Fermi level seen in Fig.~\ref{fig:fig2}(a)
translates into a suppression of the zero temperature conductance
as can be seen in Fig \ref{fig:fig2}(c). As a function of field
this quantity exhibits a peak of width $\sim \;T_{\rm K}$, as
expected from Eq.~(\ref{g-de-B}). With increasing temperature the
conductance decreases further.

The case of  negative $U_{\rm eff}$ is shown in Fig.
\ref{fig:fig2}(d). At temperatures much lower than the zero-field
value of $T_{\rm {AK}}$ we observe a wide plateau of width $\sim 2
|U_{\rm eff}|$. The region of the plateau is that in which charge
Kondo effect exists as discussed above and this leads to a high
conductance. With increasing temperature the conductance first
decreases in the central region where $T_{\rm {AK}}$ is the lowest
(see below).

At high temperatures, two peaks are seen at $B\sim\pm |U_{\rm
eff}|$. These peaks are associated to the crossing of the levels
of the isolated molecule [cf. Eq.~(\ref{eq:enes})]: for
$\left|B\right|\!>\!\left|U_{\rm eff}\right|$ the ground state of
the molecule is either $\left|\downarrow,0\right.\rangle$ or
$\left|\uparrow,0\right.\rangle$, depending on the sign of the
field. For $\left|B\right|\!<\!\left|U_{\rm eff}\right|$, instead,
the ground state of the molecule is spinless. These peaks are thus
the analogs of the familiar Coulomb blockade peaks that appear for
positive $U_{\rm eff}$ upon varying the charge. For negative
$U_{\rm eff}$ and in the electron-hole symmetric situation that we
are discussing the charge is fixed, however, and it is the spin of
the molecule that changes at the peaks by an amount $\Delta S_z =
1/2$ when the magnetic field varies.

We now discuss the spin resolved conductance at $T\!=\!0$ as a
function of gate voltage ({\it i.e.}, of $\varepsilon_d$) for the
case $U_{\rm eff}\!<\!0$ and several values of the magnetic field.
Figure \ref{fig:fig3}(a) shows the conductance at zero field. When
the molecular level departs from the symmetric position, the
molecule charge--polarizes and the conductance decreases according
to Eq. (\ref{g-de--e}). As a consequence, the conductance exhibits
a narrow peak of width $\sim \;T_{{\rm {AK}}}$.

When a small magnetic field is applied, $T_{{\rm {AK}}}$ increases
as mentioned above and the peak in the conductance broadens
accordingly [cf. Fig. \ref{fig:fig3}(b)]. There is also a spin
polarization of the current that changes sign at the symmetric
point. This can be understood as follows: for negative but small
$\delta\varepsilon_d$ the charge of the molecule increases and the
current is dominated by charge fluctuations between the states
$\left|2,0\right\rangle$ and $\left|\downarrow,0\right.\rangle$.
This leads to a predominantly spin-up current. For positive but
small $\delta\varepsilon_d$ the charge in the molecule decreases
and the relevant fluctuations are now those between
$\left|0,0\right.\rangle$ and $\left|\downarrow,0\right.\rangle$
and the spin-polarization of the current is reversed.

The width of the conductance peak further increases with the
magnetic field but the peak height remains remains nearly
unchanged as seen in Fig.~\ref{fig:fig3}(c). Notice the strong
spin-polarization of the current reflected in the strong asymmetry
of the peaks in the spin resolved conductance. In this regime the
device acts as a very effective spin filter and the spin
polarization can be reversed by a small change in the gate
voltage.
\begin{figure}[tbp]
\includegraphics[width=8.5cm,clip=true]{TKB.eps}
\caption{Magnetic field dependence of $T_{{\rm {AK}}}$ computed
from Eqs.~(\ref{eq:Jakm}) and (\ref{eq:TAK}) for the same values
of the parameters as in Fig.~\ref{fig:fig3}. The thin line is a linear fit.} \label{fig:fig4}
\end{figure}
For magnetic fields larger than the spin gap $B\gtrsim
|U_{\rm eff}|$, the ground state of the isolated molecule
changes as mentioned above and the total conductance shows a
two-peak structure. The heights of these are reduced by half as
shown in Fig.~\ref{fig:fig3}(d). These peaks are located at
$\delta\varepsilon_d \sim \pm\;\left(B -|U_{\rm eff}|\right)/2$
where there is a level crossing of the molecular states. The
conductance peaks are almost fully spin-polarized in this limit.

We conclude by discussing in detail the field-dependence of the
charge Kondo temperature $T_{{\rm {AK}}}$. As shown in Reference
\onlinecite{Cornaglia2005a}, the low-energy effective model for
the charge fluctuations in the strong {\it e--ph} phonon coupling
case is the anisotropic Kondo model with couplings $J_{\parallel}$
and $J_{\perp}$ and Kondo temperature~\cite{Costi1996, Costi1998}
\begin{equation}
T_{{\rm{AK}}} \sim \left({J_\perp/J_\parallel}\right) ^{1\over
J_\parallel \rho_0}. \label{eq:TAK}
\end{equation}

In the present case, in the presence of a magnetic field, the
coupling constants are \cite{Cornaglia2005a}
\begin{widetext}
\begin{equation}
J_{\parallel} =  \frac{J_0}{2}\!\sum_{m,\sigma\!=\!\pm 1/2}
{e^{-\left(\lambda/\omega_0\right)^2}
\left(\lambda/\omega_0\right)^{2 m}/m! \over
 {2\lambda^2/\omega_0 U} -1 -2 \sigma B/U + {2 m \omega_0/U}}\;,\;\;\; J_{\perp} =
\frac{J_0}{2}\!\sum_{m,\sigma\!=\!\pm 1/2} {(-1)^m
e^{-\left(\lambda/\omega_0\right)^2}
\left(\lambda/\omega_0\right)^{2 m}\!/m! \over
 {2\lambda^2/\omega_0 U} -1 - 2 \sigma B/U + {2 m \omega_0/U}},
\label{eq:Jakm}
\end{equation}
\end{widetext}
where $J_0\!=\!8\;\Gamma/(\pi U \rho_0)$.

For very large {\it e--ph} coupling the expressions above can be
evaluated analytically leading to the result quoted in
Eq.~(\ref{eq:deltavB}) in Sec. \ref{sec:model}. In the numerical
calculations reported here we used moderate values of $\lambda$
and the expressions for the couplings in Eq.~(\ref{eq:Jakm}) must
be evaluated numerically.

Figure \ref{fig:fig4} represents the field dependence of
$T_{{\rm{AK}}}$ for the same parameters as in Fig.~\ref{fig:fig3}.
It can be seen that in this regime $T_{{\rm{AK}}}$ still increases
exponentially with $B$.

\section{Conclusions and summary}\label{sec:conclusions}
We analyzed the equilibrium transport and spectral properties of a
model molecular transistor when the spin symmetry is broken by applying
an external magnetic field. For weak {\it e--ph} coupling, in zero
field, the conductance shows the well known Coulomb blockade peaks
at high temperature and the enhancement of the conductance due to
the Kondo effect at low temperatures. An external
 magnetic field $B\gtrsim T_{\rm K}$ suppresses the conductance as
 a result of the splitting of the Kondo peak.
 The properties of the conductance at zero bias
 are qualitatively the same as those found in the case in which there is no {\it e-ph}
 coupling but with a set of phonon renormalized parameters.
 The spectral density, however, presents a
set of additional peaks separated by the phonon energy $\omega_0$,
that can be understood analyzing the level structure of the
isolated molecule. The properties of the spectral density are
experimentally accessible in transport experiments at finite but
small source-drain voltages or in scanning tunneling microscopy
(STM) experiments for molecules on surfaces.

In the strong {\it e--ph} coupling regime the behavior of the
system is qualitatively different. The odd Coulomb blockade
valleys are completely suppressed and the low temperature physics
is dominated by charge fluctuations instead of spin fluctuations.
In a small range of gate voltages the charge Kondo effect takes
place and results in an enhancement of the conductance at low
temperatures. In contrast with the previous case, the Kondo peak
is not split by a magnetic field. Instead, for a broad range of
magnetic fields, it broadens as the latter increases. For large
enough fields or temperatures a {\it spin blockade} regime is
observed.

The magnetic field dependence of the conductance of a molecular
transistor with strong {\it e--ph} coupling resembles in many ways
the gate voltage dependence of the conductance of a device with
weak {\it e--ph} coupling in zero field. The two cases are related
to each other through the transformation $\langle \hat{S}^z_{d}
\rangle$ $\to$ $\langle \hat{n}_d \rangle$ and $B \to V_g$. This
transformation is not an exact one because the symmetries in the
spin and charge sectors of the Hilbert space are different but it
gives a good qualitative physical picture.

redpajama_set_name: RedPajamaArXiv


text:
package servlets;

import frontend.Frontend;
import org.eclipse.jetty.server.Server;
import org.eclipse.jetty.servlet.ServletContextHandler;
import org.eclipse.jetty.servlet.ServletHolder;

/**
 * @author v.chibrikov
 */
public class Main {
    public static void main(String[] args) throws Exception {
        Frontend frontend = new Frontend();

        Server server = new Server(8080);
        ServletContextHandler context = new ServletContextHandler(ServletContextHandler.SESSIONS);
        server.setHandler(context);

        context.addServlet(new ServletHolder(frontend), "/authform");

        server.start();
        server.join();
    }
}

redpajama_set_name: RedPajamaGithub


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text:
Bahrain /
87% (women 84%, men 89%)
Education index:
Internationally ranked: 0%.
$1,500/capita, 3.9%/GDP.
Formal education was introduced in Bahrain already in 1919, with the opening of boy's school in Al-Muharraq. The first girl's school opened in 1928.
Elementary schooling was for long voluntary by law, but a high percentage of boys and girls attended school. It is first in recent years that it has become compulsory.
Bahrain has proven relatively successful in creating an education system that produces candidates with relevant skills for the job market. The system also seems to produce candidates with creativity and entrepreneurial spirit.
Although girls today attend school at the same numbers as boys, Bahraini schools are strongly segregated between the sexes. This to the level that many specializations are only open for one sex.
The size of expenditure on education compared to GDP is presently highly uncertain, the last good estimate goes back to 1991, when 3.9% was used. There is, however, no doubt that Bahrain puts serious efforts into offering a good school.
Literacy and Adult education
Literacy rates in Bahrain are fair, and about in the middle compared with other countries in the Gulf region. There remains a difference between men and women, and while the gap is smaller than most other MENA countries, it is among the largest in the Gulf region.
There were in 2000 67 adult education centers, most aiming at reducing adult illiteracy.
There are also special training programs for adults with little schooling, or those in the need of vocational training for new professions. These programs offer instruction in foreign languages, courses in auto mechanics, electrical appliance maintenance, art, family life and office and secretarial skills.
Bahrain has several teaching institutions for individuals with handicaps, principally blind, deaf and the dumb.
Bahrain has both kindergartens and pre-primary schools.
Only recently was primary education made compulsory in Bahrain. Before this, schools were still well-attended, schools were easily accessible to the citizens and there was a common sharing in the understanding of schools benefitting all.
After today's system, primary education start at the age of 6 and lasts 6 years. The next level, the Intermediate, lasts 3 years and is attended by about 95% of all eligible. Until the 1980's, drop-out rates for girls were high, today, attendance is equal between the sexes at this level.
Schools in Bahrain are separated between the sexes, and although attendance for girls is equal to that of boys, there are by far more schools dedicated to boys. As this means that there are less pupils at each boy school, it reflects that education for boys is considered more important in modern-day Bahrain.
Education is Bahrain is free not only with respect to tuition, also supplies, school uniforms and meals are provided for by the state.
Primary schools have tuition in Islam, Arabic, as well as as basic science and technology, social studies, art, physical education and music. The principal language of instruction is Arabic, English is first introduced as a subject in the 4th grade, but becomes gradually also a language of tuition.
There is a designated educational program with great focus on Islam available, but only 1.5% of the total number of pupils follow this, and then only boys.
Around 60% of teachers are female, and many teachers in Bahrain schools are Egyptians.
Immigrant groups often have their own schools, providing education in native language according to national educational plans. This especially applies to Pakistanis and Indians.
About 85% attend secondary education, which lasts 3 years. Its programs are divided into: General; Industrial; and Commercial. Beyond this, there are many specializations, like science, literary studies, agriculture, printing, textiles and advertising. Specific programs are only open to one sex: most technical and vocational programs are limited to boys, textiles and advertising to girls.
About 25% of teachers at this level are non-Bahraini citizens, but this number is on the decrease. In 2000, there were 17 general secondary schools, 4 technical and 3 commercial.
Evaluation at completion of the secondary level is a combination of grades from school and the results from national exams.
Bahrain's first university came from a 1986 merger between the University College and the Gulf Polytechnic, institutions dating back to the 1960's. Arab Open University, which also has branches in the other Gulf countries was established in 1979, and these two were the only universities until 3 more were founded in the 2000's. Another important institution is the Bahrain Training Institute.
Studies at foreign universities is encouraged by the Bahraini state, there are specific programs with scholarships for the most gifted students.


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In order to obtain loan borrower should fill out simple form on this web site. We partner 100+ lenders and make it possible to design search for Payday Loans Online in Paterson New Jersey, with minimum requirements to the package of documents. All you ought to do is fill out quick online form that we have provided, then you will have an extraordinary opportunity to borrow money from 100 up to 1000. Need Emergency Loan Paterson (NJ) ZIP 7501 can promise you a safe deal.
After you submit your information we can connect you with a lender in Paterson NJ.
Direct Payday Loan Lenders Only in Paterson NJ - solution for every financial disaster! Nowadays, financial difficulties may badly affect literally everyone. Even if the hole in budget is connected with contingencies at work, problems with repayment of loan debts or financial disaster caused by the loss of your wallet, there is absolutely no point of worrying. Decision for this trivial problem can be provided by the Cash Time Personal Loans in Paterson (Passaic) NJ, ensuring the return of all of the New Jersey Payday Loans Online amount from the salary earned in the next month.
Despite the long list of benefits debtor may meet some difficulties in case of delinquency: high penalties, full payment requirement, transfer to "black list" etc. Anyway, Payday Loans Online in Paterson NJ is the optimal source to get small amounts before salary, to cover mortgage, regular payments or to prevent credit card freezing in New Jersey.
What does "Need Emergency Loan in Paterson NJ" stand for?
As mentioned above, the sum of the loan is relatively slow (up to $1,000) so it can't help one to cover college expenses, to start a business or to buy a house. Commonly Perkin Loan Payday Loans Online in Paterson NJ used to pay bills and taxes, buy presents before salary day, etc. Unlike Loans For Poor Credit , these deals are meant to help people who need small sums of money and are able to return the money in a short period of time.
This sort of commendation opportunity has the highest acceptance type, because the epitomize of the allowance is secured with borrower's return. Even imperfect credit reputation is not an obstacle for getting access to this kind of financial service. The time terms of the deal are usually selected by the clients. Most short-time personal credits are for 1-4 weeks.
What is the qualification for Payday Loans Online in Paterson NJ?
Again the obligee in Paterson NJ may ask for some additional information to be sure that lending resources to the applicant is unimperilled. For example, one can be asked to prove income additionally by sending pay stubs. This can make the procedure a little longer, because paperwork like scanning or taxing takes time, but still the answer will be given in a short period of time.
All the gathered data is encrypted and all the private information is securely protected. Every client's privacy is guarded on the highest on the up. When one makes a request for a Unsecured Loans With Bad Credit, the company needs to gather personal information on the perspective client in order to decide whether it is safe or not to provide the credit.
Most of the procedures required to check applicant's in New Jerseypersonal information, make a decision and lend the money are performed online. This option helps to make payday loans the fastest type of credits. You can fill and send your application anytime, because online services work 24/7 in Paterson (NJ). Filling out the form doesn't take much time, too: due to small amount of required information, one can finish the form in a couple of minutes. Then it takes about an hour to connect the perspective client with a lender in Paterson NJ.
If the direct deposit option is unavailable, but other criteria match, the experts can offer some other options. In most cases, it doesn't take more than one business day to receive the money after filling up and sending the form. After that, it only takes about one business day to transfer the money to the borrower's bank account. The accommodation in Paterson state New Jersey agreement is provided as soon as the final decision on the loan is made. In future the request can be easily repeated if necessary. After that the client can read the offer and decide whether to agree on the credit terms or to reject them. Rejecting the credit doesn't require any special procedures: one should just ignore the offer. If one does agree on the terms of the advance, the next step is signing the agreement with an e-sign.
Does an applicant with a unhappy credit history has a chance to be approved?
Since Payday Loans Online in Paterson NJ are secured by the regular income of the borrower, bad credit history doesn't affect much on credit decisions. Though some lenders prefer to work in traditional ways and need to perform verifications on every credit with traditional bureaus, others only check if the perspective applicant has no enormous debts with other Need Emergency Loan lenders or is not a bankrupt. That doesn't mean the credit history doesn't matter at all: low credit score can affect the terms and amounts of loan offers. But it doesn't prevent an applicant from being approved to don a accommodation.
Why is it necessary to contact loaner in Paterson NJ directly?
Our matching service provides perspective clients 24-hour access to the most reputable lenders. We make sure that our users get the best credit options. However, lenders in New Jersey don't give us detailed information on their terms regarding every particular Paterson Payday Loans Online, and those may differ. Our specialists do not make decisions on whether to give faith to the applicant, too. That's why it's easier for the borrowers who used our service and are having any issues regarding their personal contracts to speak to the companies directly.
Sometimes given Payday Loans Online in Paterson NJ need to be renewed. Why?
There are a lot of unforeseeable circumstances which can prevent borrowers from covering their debts in time. Most of the lenders easily accept this if the borrower keeps in touch and propose to renew Emergency Cash Advance for additional interest that is added to the total. One should know that this is not a cheap option. It can increase a Loans For Bad Credit debt to the sizes which will be much harder for the borrower to repay. Please make sure to prevent these circumstances by contacting the lenders as soon as you can and informing them that you've got unexpected problems. One should also know that not all states allow renewals. Check the laws of your state on Payday Loans Online in Paterson NJ before trying to renew your lend.
Additional fees and penalties can vary from deal to deal, so one should carefully read contract every time before accepting it, not only the first one. If one feels the penalties are too harsh, it may be a better choice to refuse from taking the loan. All of our Paterson lenders are known for the most honest and soft conditions on the Payday Loans Online in Paterson NJ, but that doesn't mean one shouldn't take own responsibility and think about consequences before signing the agreement. Applicable penalties, collection practices and all the additional fees for failing to pay off in time are explained in every individual loan agreement together with the cases of defaulted payment terms. This agreement should be read carefully and attentively by every applicant who wants to get a Perkin Loan. It is highly not recommended to sign the agreement without checking the terms. To keep up your cash flow, file for unemployment insurance as soon as possible. While unemployment checks won't replace all of your lost income, they will provide some assistance.
Payday Loans Online Paterson NJ are quite common way of borrowing nowadays as the required sum of money may be furnished to the consumer with a full power in a brief period of time. The process of requesting the Payday Loans Online in Paterson NJ does not need more than several minutes, the only thing to be provided by the applicant is filling up an application with correct and valid personal information and wait till the decision on the express probity will be adopted. Regardless, the investor wanted out of the stock, but had been reluctant to sell because of the capital gains. A second scenario might involve a recent retiree who owns highly appreciated shares of a growth mutual fund purchased over the course of his working life.
How much money can I get and how much does it cost? Advances range of Next Payday Loan is from $100 to $1000 in Paterson (NJ). You choose the amount of money you need depending on your financial situation. Perkin come Perkin two primary forms - fixed rate and adjustable rate - with some hybrid combinations and multiple derivatives of each. A basic understanding of interest rates and the economic Loan that determine the future course of interest rates can Loan consumers make financially sound mortgage decisions, such as making the choice between a fixed-rate mortgage or adjustable-rate mortgage ARM or deciding whether to refinance out of an adjustable-rate mortgage.. Generally finance charge which is the cost of the Payday Loans Online may range from $10 to $30 for every $100 that you borrow. As it was already mentioned, if you repay the loan before the determined term you can save some money paying only for the days you borrow.
Payday Loans Online Paterson NJ are pretty convenient due to the possibility of online service. Your loan can be funded as closely as on the same business day. The name of the lend itself means that money is given to your next salary. Loan you cannot answer a definitive "yes" to these, it would be best to simply create an overall ePrkin allocation in line with your age, and from there invest in Perkin few managed funds to start.. Notice that the amount of money you can borrow the dues you are charged can be influenced by state New Jersey laws and a lot of other factors.


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