text:
super furry animals 90s
24 respectively: these releases were the first to feature cover art from Pete Fowler, who went on to design the sleeves of all their releases up until 2007's Hey Venus. [20], Super Furry Animals reconvened for one performance on 29 February 2012 at Cardiff City Stadium before a Wales v Costa Rica Gary Speed Memorial Match, in tribute to the late Welsh footballer and team manager. Since their formation, the band has consisted of Gruff Rhys (lead vocals, guitar), Huw Bunford (lead guitar, vocals), Guto Pryce (bass guitar), Cian Ciaran (keyboards, synthesisers, various electronics, occasional guitar, vocals) and Dafydd Ieuan (drums, vocals). Super Furry Animals were formed in 1993 in Cardiff, Wales by Gruff Rhys (lead vocals, guitar), Huw Bunford (lead guitar, vocals), Guto Pryce (bass guitar), Cian Ciaran (keyboards, synthesizers, various electronics, occasional guitar, vocals) and Dafydd Ieuan (drums, vocals). All the singles and albums of SUPER FURRY ANIMALS, peak chart positions, career stats, week-by-week chart runs and latest news. The lyrics on all the tracks on both EPs were in Welsh, except for "God! [15] The album's first single, "Show Your Hand", failed to enter the top 40, their first to do so since 1996's "Hometown Unicorn", despite modest airplay. Over the course of nine albums, Super Furry Animals have been described as "one of the most imaginative bands of our time"[3] by Billboard, while according to a 2005 article in NME, "There's a case to be argued that [Super Furry Animals] are the most important band of the past 15 years".[4]. 3 in the album charts. "[19], In 2010, Super Furry Animals went on what became a five-year hiatus, as bassist Guto Pryce revealed in an interview with Wales Online. Super Furry Animals were one of the first post-alternative bands, fusing together a number of disparate musical genres -- including power pop, punk rock, techno, and progressive rock -- creating a shimmering, melodic, irreverent, and willfully artsy rock & roll. 13th May 2016. 2:14 … Fuzzy Logic, although stylistically closer to Britpop than any other Super Furry Animals album, is ultimately too creative and frankly, too clever, to be lumped in with a scene that spent far too much time looking back, and nowhere near enough time looking forward (and yes, given I am Backseat Mafia's resident 'Not Forgotten' writer, I am fully aware of my level of hypocrisy here). Drummer Ieuan formed a band known as The Peth which has been described by Rhys in various magazine articles as "Satanic Abba": the band also reunites Rhys Ifans with the SFA family, as he takes lead vocal duties. When they managed this, there was no upcoming release to attach it to – so it came out as a limited edition single in its own right, in December 1996. The album, released the same month, sold remarkably well for a non-English LP – it made No. The Best of 1995–2016, was released on 4 November 2016. 28): neither had that much impact but still received some airplay, notably on BBC Radio 2. According to drummer Dafydd Ieuan: "It all started when we played this festival in West Wales, and for some reason the Welsh media started foaming at the mouth because we were singing songs in Welsh and English. Another single, "Hello Sunshine", hit No. View all records by Super Furry Animals for sale on CDandLP in LP, CD, 12inch, 7inch format. In a Melody Maker interview, Super Furry Animals said the "Smokin'" referred to smoking haddock, or to truck drivers' tyres when they're 'burnin' the roads'. Although the reviews for the album were generally good and it sold well initially, charting at No. When Super Furry Animals's first album, Fuzzy Logic, was released in 1996, it introduced a Britpop-enthralled audience to a band who had only the loosest interest in … Lyrics to 'Ymaelodi Âr Ymylon' by Super Furry Animals. Information on Super Furry Animals. Super Furry Animals are a Welsh rock band formed in Cardiff in 1993. Can you name the released songs by Super Furry Animals? The ceremony took place on the day after the terror attacks on the World Trade Center and the Pentagon, and SFA's performance of the album track "It's Not the End of the World?" The following albums feature tracks by other artists chosen by one or more of the Super Furry Animals. Formed when techno DJs Rhys Ifans, Daffyd Ieuan and Guto Pryce teamed up with local songwriter Gruff Rhys in 1993, Super Furry Animals came to recognition during the Brit-pop era and survived as c.. Super Furry Animals. BBC Wales's Sports Correspondent Bob Humphrys reports on the unique kit deal: The Super Furries agreed a five-figure sum to back the Bluebirds in their FAW Cup run this season. Also (for the CD edition) a second disc, containing a sackful of previously unreleased material. Super Furry Animals. And since their formation in the early 90s, the Super Furry legend has become something of a cliché: the blue techno tank, the 40ft inflatable bears, the record-breaking debut release, the song with that title. Super Furry Animals and Owen produced the group's debut album, which was preceded by two singles in the spring of 1996 -- "Hometown Unicorn" and "God! His first solo album, Yr Atal Genhedlaeth preceded his band's LP, Love Kraft, in winter '05. The album's cool commercial reception (it charted at just No. Fuzzy Logic, the band's debut album, was released in the U.K. in June 1996 to uniformly excellent reviews and a place in the Top 40. Additionally, the album Rings Around the World was released with low-budget videos accompanying each track. However, they had established themselves as favourites in the music press, a cut above the majority of their Britpop peers. Favourite Add to Gruff Rhys | A3 Digital Print | Limited Edition of 100 KrakajacPaperCo. Super Furry Animals released their lively wild-ride album Fuzzy Logic in 1996, throwing some Welsh weirdness into the Britpop mix. Pryce noted that the band expected to reconvene as soon as the members finished with the various projects they were working on. Listen now Super Furry Animals (1995) Cerys Matthews sy'n cyflwyno sesiwn Super Furry Animals o raglen Heno Bydd Yr Adar Yn Canu (15/01/1995). In September 2018, the official Super Furry Animals Twitter feed posted an announcement[29] of a multi-disc set of recordings made at the BBC to be released on 23 November 2018. Complete your Super Furry Animals collection. View all records by Super Furry Animals for sale on CDandLP in LP, CD, 12inch, 7inch format 22 in the charts and became Super Furry Animals' standard closing number when they played live. This is another two-CD set and contains a mix of singles, album tracks, band favourites, B-sides and more. 1. Das Koolies released their debut single "It's All About The Dolphins" on 29 January 2020. Cerys Matthews introduces Super Furry Animals … seemed to be an attack on the complacency of organised religion. The same month a biography, Rise of the Super Furry Animals, was published by HarperCollins. Super Furry Animals Dec 17 2016 Artist: Super Furry Animals , Tour: Fuzzy Logic and Radiator 20th Anniversary , Venue: Motorpoint Arena Cardiff , Cardiff , Wales January 2000 involved a series of changes for SFA. However, Super Furry Animals regarded "The Man Don't Give a Fuck" as one of their best songs and continued their efforts to clear the sample. Formed in Cardiff, Wales, in 1993, Super Furry Animals were comprised of Gruff Rhys (lead vocals, guitar), Huw "Bunf" Bunford (guitar, vocals), Guto Pryce (bass), … The laid-back ambience recalls early-1970s Beach Boys albums such as Surf's Up (which SFA have referred to as one of their favourite albums), whilst the heavy use of strings suggested the likes of Scott Walker and Curtis Mayfield. The Best Of Super Furry Animals 1995-2016. Mae'n hnw'n dweud bo' ni ar yr ymlon They say we're peripheral people Yn weiston bach ffyddlon, yn arw ac estron Spineless and feeble, roughneck and evil Ac mae hi'n llugoer yn llygad y ffynnon Since their formation, the band has consisted of Gruff Rhys (lead vocals, guitar), Huw Bunford (lead guitar, vocals), Guto Pryce (bass guitar), Cian Ciaran (keyboards, synthesisers, various electronics, occasional guitar, vocals) and Dafydd Ieuan (drums, vocals). The Official YouTube channel of Super Furry Animals, the Welsh psychedelic pop band featuring Gruff Rhys, Cian Ciaran, Dafydd Ieuan, Huw Bunford, Guto Pryce. Available in standard sizes. The Moog Droog EP followed in October 1995, named after the synthesiser manufacturer Robert Moog and the Nadsat term for "friend" in A Clockwork Orange. Featuring four tracks, the EP sampled from Black Uhuru. This ultimately cemented its legendary status and did much to establish Super Furry Animals as cult heroes, as the song contained the word "fuck" over 50 times and therefore received practically no airplay. During this time some of the bands' music was used prominently in The Rock-afire Explosion documentary movie, namely Hello Sunshine and Some things Come From Nothing. 16). It is cited by many critics and fans alike as their most polished and accessible work. Gruff Rhys is the lead singer of the Welsh band Super Furry Animals. Special offers and product promotions. Compilation album featuring tracks picked by the Super Furry Animals. It was nominated for the Mercury Music Prize in 2001. He performs solo and with several bands, including Super Furry Animals who obtained mainstream success in the 1990s. Using the psychedelicized prog-punk of Fuzzy Logic as a foundation, Super Furry Animals move even further into left field on their second album, Radiator. that will be released this September. 8: however, Creation did not serve the album particularly well by releasing it just four days after the long-awaited new effort from Oasis, Be Here Now. Super Furry Animals tabs, chords, guitar, bass, ukulele chords, power tabs and guitar pro tabs including god show me magic, misunderstanding, demons, northern lites, the man dont give a fuck Super Furry Animals are a Welsh rock band formed in Cardiff in 1993. Using the psychedelicized prog-punk of Fuzzy Logic as a foundation, Super Furry Animals move even further into left field on their second album, Radiator.As before, the group displays a gift for catchy, deceptively complex melodic hooks, but now its songwriting and arrangements are mind-bogglingly intricate and eclectic. Super Furry Animals. 23 in the charts, but it garnered a little more interest when next single "Something 4 the Weekend" (a reworked, more mellow version of the album track) was given considerable radio airplay and charted at No. After Bunford and Ciaran (Ieuan's younger brother) joined, they wrote some songs, and in 1995 signed to Ankst, a Welsh indie label. Electronic collage of old Beatles recordings. Subscribe for news and competitions. [5] The band has also made reference to Blur, Elvis Costello, and Wynton Marsalis as major influences in their work. But that's doing lazy justice to their undoubted genius, for they're simply one of the most exciting and innovative groups to have ever emerged in Wales. However, there were problems in clearing a sample from "Showbiz Kids" by Steely Dan which formed the basis of the chorus, and it was switched for a different track. This is one of the most colorful and creative records of the Cool Cymru movement. A limited edition (of 3000) 7 inch record, "Ysbeidiau Heulog" (meaning "Sunny Intervals") preceded Mwng in May 2000. Super Furry Animals were formed in 1993 in Cardiff, Wales by Gruff Rhys (lead vocals, guitar), Huw Bunford (lead guitar, vocals), Guto Pryce (bass guitar), Cian Ciaran (keyboards, synthesizers, various electronics, occasional guitar, vocals) and Dafydd Ieuan (drums, vocals).[1]. Super Furry Animals, much like Manic Street Preachers, deserve way more attention outside of the United Kingdom. Overview ↓ Biography ↓ Discography ↓ Songs ↓ Credits ↓ Awards ↓ Related ↓ Share on facebook; twitter; tumblr; Credits (1-266 of 266) Year Album Artist . 3. In May, their debut album Fuzzy Logic was released, to wide critical acclaim. [30], 2017–present: Second hiatus and Das Koolies, Last edited on 13 December 2020, at 06:05, "Super Furry Animals Announce New Box Set Covering Years of BBC Sessions", "Super Furry Animals : Love Kraft (review)", "Oasis manager Alan McGee tells his rock 'n roll story", "The Super Furry Animals: When Paul McCartney played the celery", "Super Furry Animals – Super Furry Animals Happy To Turn Down Coke Deal", "Super Furry Animals plan 'speaker blowing' comeback", "Super Furry Animals – Dark Days/Light Years (review)", "Super Furry Animals: Dark Days/Light Years", "unofficially super furry animals - sfa - News", "Welsh rock icons Super Furry Animals to launch their own beer", "Super Furry Animals Share Video for New Song "Bing Bong, "Super Furry Animals to return after seven years with Euro 2016 anthem 'Bing Bong, "Caught by the River Thames festival review – a maverick lit-rock-nature fete", "Super Furry Animals to play Fuzzy Logic and Radiator back-to-back", "Release Info: Super Furry Animals at the BBC 23/11/2018", Super Furry Animals biography from BBC Wales, https://en.wikipedia.org/w/index.php?title=Super_Furry_Animals&oldid=993927827, Creative Commons Attribution-ShareAlike License, This page was last edited on 13 December 2020, at 06:05. Explore releases from Super Furry Animals at Discogs. Electronic collage of out-takes from Beatles recording sessions along with several audio recordings made by Paul McCartney including "sounds of the, Her Space Holiday album featuring remixes of tracks from. [22][23], In May 2015, the band played several gigs from early May to September to accompany a major reissue of their 15-year-old album Mwng, which had been out of print. D G | Gm6: 310030 / Hello sunshine | repeat (2x) F#m7: 242222 / D G | G6: 020030 / Come into my life | A7sus4: 002030 / CHORUS: D Em G A / in honesty it's been a while / D Em G A / since we This was a collection of songs from the 1995 Ankst releases (including "Dim Brys: Dim Chwys"), the band's favourite B-sides, plus "The Man Don't Give a Fuck" and "Smokin'". The band also selected tracks for a volume in the Under the Influence series of compilations, in which artists present the songs that they feel have most contributed to their sound. In February 1996, the band's debut on Creation, "Hometown Unicorn", became New Musical Express's Single of the Week, chosen by guest reviewers Pulp, and the first Super Furry Animals single to chart in the UK Top 50, peaking at No. 18 in July 1996. [16] The album's progress was recorded in a series of short films that were shown on the band's website in the build-up to the release. If ludicrous publicity stunts and crazed rock and roll adventures are your thing, Rise of the Super Furry Animals by Ric Rawlings will deliver plenty of hair-raising laughs. Find out at which radio station you can hear Super Furry Animals - Fix Idris Super Furry Animals - Fix Idris - Listen on Online Radio Box This site uses cookies . [6], The earliest Super Furry Animals track commercially available is "Dim Brys: Dim Chwys", recorded in 1994 for Radio Cymru: an ambient piece, the track shows the band's techno roots. Show Me Magic", charted at No. 33 upon release in April 1996 and also became NME single of the week. They accompanied this with a download single, "Slow Life", which also included the track "Motherfokker", a collaboration with Goldie Lookin Chain, both tracks are now available as a free download via the Placid Casual website. Super Furry Animals Biography by Stephen Thomas Erlewine + Follow Artist. 1, accompanied by a single – a live version of "The Man Don't Give a Fuck" (chart No. Rawer than the "Moog Droog" version, it clocks in at 1 min 50 secs. Actor Rhys Ifans is a former member. [21], In 2014, craft brewer The Celt Experience created a tribute "Fuzzy Beer" in collaboration with the band. On Love Kraft this was no longer the case, as Rhys, Bunford, Ieuan and Ciaran all contributed songs and lead vocals. 4, the album broke little new ground by SFA's standards and the band had fallen out of fashion, receiving little coverage in the music press. 11 in the charts – and received a rare distinction for a pop record, being commended in Parliament for its efforts in keeping the Welsh language alive.[10]. 1996 Super Furry Animals: If You Don't Want Me to Destroy You (Video short) (performer: "If You Don't Want Me to Destroy You") EastEnders (TV Series) (performer - 1 episode, 1996) (writer - 1 episode, 1996) He was a drummer for Welsh band Catatonia from 1993-1996, recording on their early singles and debut album Way Beyond Blue released in 1996. Ready for your walls, shelves, and the world. He formed the electro-pop outfit Neon Neon with Boom Bip. This was the Ice Hockey Hair EP, widely held as one of their finest moments. 30), following "(Drawing) Rings Around the World" (chart No. During the same period Super Furry Animals formed and Ieuan left Catatonia to focus on them. The final tour of their reunion, in which they played both Fuzzy Logic and Radiator in full across the UK and Ireland, took place in December 2016.[28]. The eccentric experimental rock of the Super Furry Animals has proven consistently brilliant over a 15-year career that has spawned eight wildly inventive albums. Ciaran's side project Acid Casuals released their debut album Omni in January 2006 on the Placid Casual label. 19) suggested that they had returned to their familiar status of critically acclaimed cult favourites. Two singles preceded the new album, "Hermann ♥'s Pauline" in May and "The International Language of Screaming" in July, hitting No. The reviews were, if anything, better than those for Fuzzy Logic, and it sold more quickly than its predecessor, reaching a peak of No. ... 90s Rock Songs by 5 Words 138; 300 Kpop Faves On Shuffle 2 115; NCT age in order 80; Name All 23 NCT Members (SPEED QUIZ) 72; In January 2016, the band announced their first North American tour in six years. 25. The Fuzzy Logic deluxe and the new compilation are out on 4 November 2016. 9. All the singles and albums of SUPER FURRY ANIMALS, peak chart positions, career stats, week-by-week chart runs and latest news. With the purchase of a CD or Vinyl record dispatched from and sold by Amazon, you get 90 days free access to the Amazon Music Unlimited Individual plan. 28). [2], Super Furry Animals have recorded nine UK Albums Chart Top 25 studio albums (one BPI certified Gold and four certified Silver), plus numerous singles, EPs, compilations and collaborations. 20. 5 out of 5 stars (51) 51 reviews £ 11.99. Rings Around the World is also remarkable for being the world's first simultaneous release of an audio and DVD album. In November 1998, the album Out Spaced was released. It came backed with "Charge", a hard-rock jam recorded as a Peel Session for the BBC. 12 in the charts and leading to a memorable appearance on "Top of the Pops". High quality Super Furry Animals inspired art board prints by independent artists and designers from around the world. took on a somewhat bitter edge. They formed in Cardiff, Wales in 1993 by… read more Super Furry Animals are a Welsh rock band formed in Cardiff in 1993. 03. Professionally printed on watercolor textured boards. Can you name the released songs by Super Furry Animals? Love Kraft was also the last album released under Epic Records, as their contact expired in early 2006. The sixth solo album from Super Furry Animals frontman Gruff Rhys is typically internationalist in its outlook. Arranged By – Super Furry Animals (tracks: 1-1, 1-2, 1-4 to 1-14) Engineer – Michael Brennan Jr. , Nick Addison Show Me Magic" -- which became moderate hits. SFA finished their UK tour at the Cardiff International Arena in Cardiff, where they showcased the first ever concert in surround sound and broadcast it on the World Wide Web. 1 Something 4 the Weekend. A limited edition appeared in a comedy rubber sleeve, shaped like a nipple. The band are considered to be part of the renaissance of Welsh music (and art, and literature) in the 1990s: other Welsh bands of the time include the Manic Street Preachers, Stereophonics, Catatonia and Gorky's Zygotic Mynci. This twentieth anniversary reissue includes the remastered album plus a round-up of all the contemporary B-sides. Later in March, they performed the record in its entirety through an exclusive stream on their website. Guerrilla Super Furry Animals. The discography of Super Furry Animals, a Welsh indie rock band, consists of nine studio albums, four extended plays, twenty three singles and three video albums. When Super Furry Animals's first album, Fuzzy Logic, was released in 1996, it introduced a Britpop-enthralled audience to … Gruff; born 18 July 1970 in Haverfordwest is a Welsh musician, composer, producer, filmmaker and author. Supper-Furry-Animals.jpg. Their new album is far from a retread of past ideas. The next album, Phantom Power, relied less on sound experimentation and proved to be a more stripped-down, back-to-basics recording in contrast to the orchestral Rings Around the World. Find out at which radio station you can hear Super Furry Animals - Fix Idris Super Furry Animals - Fix Idris - Listen on Online Radio Box This site uses cookies . In their own way Super Furry Animals are great show men, but the characters we developed – and have done since – seemed to almost become part of the band, take some of the attention off them and let the music do the talking. The album swung from glam and garage rock numbers ("Night Vision", "The Teacher") to novelty techno ("Wherever I Lay My Phone (That's My Home)"), ambient indietronica ("Some Things Come From Nothing") and upbeat drum and bass ("The Door To This House Remains Open").
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\section{Introduction}

Recent studies have found that transport in multi-band semimetals is substantially different from conventional transport based on the classical Boltzmann theory. This is due to the particle-hole (PH) symmetry, which is realized, at least approximately, in multi-band systems when the Fermi energy is between two neighboring bands. A typical example is
the Dirac node of graphene. The PH symmetry of this two-band model leads to characteristic quantum effects, such as spontaneous particle-hole pair creation on arbitrarily small energy scales, which are only limited by the band width of the material. This is accompanied by strong fluctuations (also known as ``zitterbewegung''), which causes a finite dc conductivity even in the absence of disorder. Although graphene is a two-dimensional (2d) material, where fluctuation effects are strong, these quantum fluctuations may also play a crucial role in higher dimensions. Based on this idea, there has been a lot of progress to compute transport properties in systems like the 3d Weyl semimetals
\cite{PhysRevB.33.3257,PhysRevB.33.3263,PhysRevB.83.205101,PhysRevLett.106.056401,
PhysRevB.84.235126,PhysRevLett.107.186806,PhysRevLett.108.140405,PhysRevLett.108.046602,
PhysRevB.85.195320,PhysRevB.86.115208,PhysRevB.85.035103,PhysRevB.87.235306,PhysRevB.89.014205,
PhysRevLett.110.236803,PhysRevB.87.155123,PhysRevLett.112.016402,PhysRevB.89.054202,
PhysRevB.90.241112,PhysRevLett.113.026602,PhysRevLett.114.166601,Ziegler2016,pixley2021rare}.

The fundamental quantity for the study of quantum transport is the transition probability $P_{{\bf r}\br'}$, for a particle to move from site ${\bf r}'$ to a site ${\bf r}$ on a $d$-dimensional lattice. This classical quantity can be linked to a quantum model through the average two-particle Green's function (A2PGF) of a particle of energy $E$, given by
\begin{equation}
K_{{\bf r}\br'}=\frac{1}{\pi}
\left \langle G_{{\bf r}\br'}(E+i \,\epsilon)
\,G_{{\bf r}'{\bf r}}(E-i\, \epsilon)\right \rangle_d
\ \ \
( \text{where } \epsilon>0)\,.
\label{2pgf}
\end{equation}
Here $H$ is a random Hamiltonian,
$G_{{\bf r}\br'}(E+i \,\epsilon)=\left \langle{\bf r}'|(H-E-i \,\epsilon)^{-1}|{\bf r}\right \rangle$
is the one-particle Green's function, and $\left \langle \ldots \right \rangle_d$ denotes averaging with respect to disorder-induced randomness. Then the transition probability is given by
$P_{{\bf r}\br'}=K_{{\bf r}\br'}/\sum \limits_{{\bf r}'}
K_{{\bf r}\br'}$. The time-dependent transition probability
is obtained through the Fourier transformation $E\to t$.
The transport properties in the metallic regime can be understood by computing the diffusion coefficient $D$, which can be obtained from $K_{{\bf r}\br'}$ as~\cite{THOULESS197493}
\begin{equation}
D=\lim_{\epsilon\to0}\epsilon^2\sum \limits_{{\bf r}\in \Lambda} r^2  \,K_{0 {\bf r}}\,,
\label{diffusion_coeff00}
\end{equation}
on a lattice $\Lambda$. The corresponding dc conductivity is related to $D$ via the Einstein relation.

We can assume that the form of $G$ results from a self-energy approximation in interacting many-body systems. Then $\epsilon$, as the imaginary part of the self-energy, depends on the
frequency $\omega$ and the Fermi energy $E_F$. With this, we can bridge the microscopic quantum modeling and the more qualitative hydrodynamic description of transport due to long-lived modes in quantum systems~\cite{PhysRevB.76.144502,LUCAS2015239,PhysRevD.89.066018,hartnoll2018holographic,ips_andy}. In particular, using this formalism, we can analyze the effect of a vanishing $\epsilon \sim \omega^s$, where $s$ is a positive rational number.

In this paper, we will focus on diffusion in systems with PH symmetry, in the
presence of disorder. We assume that the disorder also obeys the PH symmetry. Although systems without
PH symmetry can also be treated by the subsequently discussed method (cf. Refs.~~\cite{PhysRevB.86.155450,Ziegler2013}), we shall focus here only on the PH-symmetric case for simplicity.
Taking into account the fact that averaging over a random distribution
of disorder leads to spontaneous PH symmetry-breaking, we employ a field theory representation to study this effect. Although the PH symmetry is discrete, an underlying global symmetry of the field theory is continuous \cite{PhysRevB.79.195424}. Thus, there is a massless mode associated with the spontaneous PH symmetry-breaking that leads to long-range correlations. These correlations are the origin of diffusion. They can be calculated from the massless mode, using the integration over the symmetry related saddle point manifold. This is known as the integration with respect to the invariant measure of the symmetry group, and is often approximated in a leading order gradient expansion, also known as the nonlinear sigma model approach \cite{WEGNER1987210}.
Here we will consider the full invariant measure, which was shown to provide a simple expression for the  A2PGF in terms of a random-phase model \cite{Ziegler_2015}.
This is briefly summarized in Sec.~\ref{sect:rpa}.

The paper is organized as follows. The representation of the invariant measure by the random-phase model is briefly reviewed in Sec.~\ref{sect:rpa}. In Sec.~\ref{sect:fir}, we introduce a fermionic functional integral for the description of the A2PGF, and employ a perturbation expansion around the diffusive approximation. It is shown that one- and two-loop corrections vanish, indicating the robustness of
diffusion. In Sec.~\ref{sect:discussion} we study some examples of the microscopic Hamiltonians with PH symmetry, and the results reveal that the diffusion coefficients depend strongly on the details of these microscopic Hamiltonians.

\section{random-phase representation of the average two-particle Green's function}
\label{sect:rpa}

For simplicity, we are restricting the discussion to two bands, while an extension to $n$ bands is straightforward.
Hence, our starting point is a two-band Hamiltonian $H$ with matrix elements $H_{{\bf r} j,{\bf r}'j'}$, where ${\bf r},{\bf r}'$ are the co-ordinates on a $d$-dimensional lattice, and $j,j'$ are band indices. In this case, we can assign a Pauli matrix representation for the Hamiltonian as
\begin{equation}
H_{{\bf r} j,{\bf r}' j'}=\sum \limits_{ a=1}^3 \mathcal{H}_{a;{\bf r}\br'}\,
\sigma^a_{jj'}\, ,
\end{equation}
where $\sigma^a $ is a Pauli matrix, and $ \mathcal{H}_{a;{\bf r}\br'}$ a matrix element on the lattice.
An instructive example is discussed in Appendix~\ref{app:example}.
The ${\bf r}$-independent PH transformation $S$ transforms the Hamiltonian $H$ as $S\,H\,S^{-1}=-H$, which implies that an eigenvector $\Psi_E$ with energy $E$ is related to the eigenvector $\Psi_{-E}$ with energy $-E$ by $\Psi_{-E}=S\,\Psi_E$. Thus, $S$ is a symmetry transformation for the Green's function $G(z)\to -S\,G(z) \,S^{-1}=G(-z)$ at $z=0$, which is exactly at the mirror-symmetric point between the two symmetric bands. Due to the poles of $G(z)$, this
symmetry-point must be treated with care. We can avoid the poles by choosing $z=i \,\epsilon$ ($\epsilon>0$).
Then the difference, in the limit $\epsilon\to 0$, reads
\begin{equation}
\lim_{\epsilon\to0} \left [-S\,G(i \,\epsilon)\,S^{-1}-G(i \,\epsilon) \right ]
=\lim_{\epsilon\to0} \left [G(-i \,\epsilon)-G(i \,\epsilon) \right ] .
\label{spont.ssb}
\end{equation}
A nonzero result indicates a spontaneously-broken PH symmetry. For the diagonal elements of the Green's functions, the right-hand side is proportional to the density of states at $E=0$. This reflects the fact that a nonzero density of states at $E=0$ provides a sufficient condition for spontaneous PH symmetry-breaking.

The disorder averaged one-particle Green's function can be calculated within the self-consistent Born approximation (or the saddle-point approximation of a functional-integral representation) as
\begin{equation}
\left \langle H\pm i \,\epsilon\right \rangle_d  ^{-1}\approx
\left [H_0\pm i \left (\epsilon+\eta \right) \right ]^{-1},
 \quad
H_0=\left \langle H\right \rangle_d +\Sigma',
\label{scba}
\end{equation}
where
$\Sigma'$ is the real part of the self-energy, and $\eta$ is its imaginary part.
The parameter $\eta$ provides a broadening of the average one-particle Green's function, and
also plays the role of an order parameter for spontaneous PH symmetry-breaking, since
we get $2\,i\,\eta \left (H_0^2+\eta^2 \right )^{-1}$ for Eq.~(\ref{spont.ssb}).

Transport properties are determined by properties on large time and spatial scales.
In Ref.~\cite{Ziegler_2015}, it was shown that the long-range part of the A2PGF of Eq.~(\ref{2pgf}) can be obtained by reducing the disorder average to the integration with respect to the invariant measure of the saddle-point manifold. This means that in practice, we replace $H$ with the effective
random-phase Hamiltonian
\begin{equation}
{\cal H}_R= U \,H_0 \, U^\dagger
\ ,\ \ \
U=\text{diag}(e^{i \,\alpha_{{\bf r} j}})\,,
\end{equation}
and then average with respect to the independently and identically distributed random-phases $\{\alpha_{{\bf r} j}\}$.
This gives us
\begin{equation}
K_{{\bf r}\br'}
\sim{\cal K}_{{\bf r}\br'}
=\frac{\left \langle adj_{{\bar {\bf r}}{\bar {\bf r}}'}
\,C\right \rangle_\alpha}{\left \langle  \det C\right \rangle_\alpha}
\ ,\ \
\left \langle \ldots \right \rangle_\alpha
=\frac{1}{2\pi}\int_0^{2\pi} \ldots
\prod \limits_{{\bf r},j}d\alpha_{{\bf r} j}\,,
\label{corr1a}
\end{equation}
with the random-phase matrix
\begin{equation}
C_{{\bf r}\br'}= 2\delta_{{\bf r}\br'}-\sum \limits_{j,j'}
e^{i \,\alpha_{{\bf r} j}} \,h_{{\bf r} j,{\bf r}'j'}
\sum \limits_{j'',{\bf r}''} h^\dagger_{{\bf r}'j',{\bf r}''j''}
\,e^{-i \,\alpha_{{\bf r}''j''}}
\ ,
\end{equation}
with
\begin{equation}
h_{{\bf r}\br'}=\mathcal{I}_2 \,\delta_{{\bf r}\br'}
+ 2\,i \,\eta \left (H_0 - i \,{\bar\eta} \right)^{-1}_{{\bf r}\br'}
\,,\quad
{\bar\eta}=\eta+\epsilon\,,
\label{def_h}
\end{equation}
and $adj_{{\bar {\bf r}}{\bar {\bf r}}'} C$ denoting the elements of the adjugate matrix.
Under a PH transformation, we obtain the Hermitian conjugation $S\,h\,S^{-1}=h^\dagger$, which implies that $C$ is real and symmetric. The quantity $U\,h\,U^\dagger$ represents the effective one-particle Green's function of the generic system, while $C$ is the corresponding effective two-particle propagator.

Although $C_{{\bf r}\br'}$ is still a random matrix, the A2PGF in Eq.~(\ref{corr1a}) is much simpler to treat than the A2PGF in Eq.~(\ref{2pgf}), because the phase integration is not plagued by poles of the integrand. Nevertheless, this does not mean that the theory becomes simple. For instance, the long-range behaviour of the A2PGF is based on the zero modes of $C$, which exist for any realization of the random-phases due to the relation
\begin{equation}
h\,h^\dagger
={\bf 1}-4 \,\epsilon \left(1-\epsilon \right ){\bar\eta}
\left( H_0^2+{\bar\eta}^2 \right)^{-1}
\ .
\label{unitary0}
\end{equation}
This implies that the constant mode $\Psi_0$ with vanishing wavevector ${\bf k}=0$ obeys
\begin{equation}
\sum \limits_{{\bf r}'}C_{{\bf r}\br'}\Psi_0\sim c \,\epsilon \,\Psi_0
\ ,
\end{equation}
i.e., $\Psi_0$ is always a zero-energy eigenmode of the effective two-particle propagator in the limit $\epsilon\to 0$.

In order to evaluate ${\cal K}$, or the diffusion coefficient $D$, we can employ two
different methods. The first is based on a graphical representation, while the second involves a fermionic functional integral representation. While the former was described and
discussed in Ref.~\cite{Ziegler_2015}, we will focus on the latter in this paper.

\subsection{General properties of ${\tilde {\cal K}}_{\bf q}$}

Before we start with the specific calculations, it is useful to mention an important
connection between the two-particle and the one-particle Green's function (``Ward Identity''), which takes the form
\begin{equation}
{\tilde K}_{{\bf q}=0}=\frac{\pi}{\epsilon}\left \langle\rho(0)\right \rangle_d
\ ,
\end{equation}
after averaging. Here, $\left \langle\rho(0)\right \rangle_d$ is the disorder average of the density of states
at energy $E=0$, which is typically nonzero and finite. Although we do not
have a proof, this relation should also hold for ${\cal K}$ due to $K\sim {\cal K}$ on large scales. Therefore,
${\tilde {\cal K}}_{{\bf q}=0}\sim \text{const.} \,\epsilon^{-1}$, which will be confirmed in the subsequent calculation.
The second derivative with respect to $q_\mu$ at ${\bf q}=0$ is
\begin{equation}
-\partial_{q_\mu}^2{\tilde K}_{\bf q}\Big|_{{\bf q}=0}\equiv -{\tilde K}_0''
=D\epsilon^{-\beta}
\ ,
\end{equation}
with $\beta=2$ for diffusion. This is in agreement with Eq.~(\ref{diffusion_coeff00}).
Higher-order derivatives of ${\tilde {\cal K}}_{\bf q}$ are also of interest, since
\begin{equation}
\sum \limits_{{\bf r}} ({r_\mu})^{2n}\,K_{0{\bf r}}
=(-1)^n \,{\tilde K}^{(2n)}_0
\end{equation}
describe higher moments of spatial fluctuations.

\section{Functional integral representation}
\label{sect:fir}

The averaged determinant in Eq.~(\ref{corr1a}) can be expressed as a fermionic (Grassmann) functional integral
\cite{zbMATH01727741}
\begin{equation}
\left \langle\det C\right \rangle_\alpha = \int_\Psi \left \langle\exp(-\Psi\cdot C \,\bar{\Psi})\right \rangle_\alpha ,
\end{equation}
which implies that
\begin{equation}
{\cal K}_{{\bf r}\br'}=\frac{\int_\Psi \bar{\Psi}_{\bf r}\Psi_{{\bf r}'}\left \langle\exp(-\Psi\cdot C \,\bar{\Psi})\right \rangle_\alpha}
{\int_\Psi \left \langle\exp(-\Psi\cdot C \,\bar{\Psi})\right \rangle_\alpha} \,.
\label{prop2}
\end{equation}
In terms of a perturbation theory around $\bar{C}=\left \langle C\right \rangle_\alpha$,
with
\begin{equation}
\left \langle C_{{\bf r}\br'}\right \rangle_\alpha
=2 \, \delta_{{\bf r}\br'}-\sum \limits_{j,j'=1,2}
h_{{\bf r} j,{\bf r}'j'} \, h^\dagger_{{\bf r}'j',{\bf r} j}
=2\,\delta_{{\bf r}\br'}-Tr_2 \left (h_{{\bf r}\br'} \,h^\dagger_{{\bf r}'{\bf r}} \right ),
\label{av_c00}
\end{equation}
we have
\begin{equation}
\left \langle e^{-\Psi\, C \,\bar{\Psi}} \right \rangle_\alpha
=\left \langle
e^{-\Psi \, \left (\bar{C}-C' \right )\bar{\Psi}}
\right \rangle_\alpha
=\left [1+\left \langle \left (\Psi\, C'\,\bar{\Psi} \right )^2 \right \rangle_\alpha/2
+ \ldots
\right ] e^{-\Psi\, \bar{C} \,\bar{\Psi}}\ .
\end{equation}
Using this, we obtain
\begin{equation}
\int_\Psi \bar{\Psi}_{\bf r} \,\Psi_{{\bf r}'}\left \langle
e^{-\Psi\, C \,\bar{\Psi}} \right \rangle_\alpha
=\int_\Psi\bar{\Psi}_{\bf r} \, \Psi_{{\bf r}'}[1+\left \langle(\Psi\, C'\,\bar{\Psi})^2\right \rangle_\alpha/2 +...]
e^{-\Psi\, \bar{C}  \,\bar{\Psi}},
\end{equation}
and
\begin{equation}
\int_\Psi \left \langle
e^{-\Psi\, C \,\bar{\Psi}}\right \rangle_\alpha
=\int_\Psi \left [1+\left \langle(\Psi\, C'\,\bar{\Psi})^2\right \rangle_\alpha/2 +
\ldots \right ]
e^{-\Psi\, \bar{C} \,\bar{\Psi}}\ .
\end{equation}
After normalizing both the expressions by $Z_0=\det\left \langle C\right \rangle_\alpha$, we can represent the result
graphically by two-loop graphs as depicted in Fig.~\ref{fig:feynman} (neglecting higher order terms indicated by $ \ldots $). The square in Fig.~\ref{fig:feynman} represents the vertex
\begin{equation}
V_{{\bf r}_1{\bf r}_2{\bf r}_3{\bf r}_4}
\equiv \left \langle C'_{{\bf r}_1{\bf r}_2} \, C'_{{\bf r}_3{\bf r}_4}\right \rangle_\alpha
=Tr_2 \left ( h_{{\bf r}_1{\bf r}_2} \,h^\dagger_{{\bf r}_2{\bf r}_3}
\,h_{{\bf r}_3{\bf r}_4} \,h^\dagger_{{\bf r}_4{\bf r}_1} \right )
-\delta_{{\bf r}_1{\bf r}_3} \sum \limits_j
\left (h_{{\bf r}_1{\bf r}_2}\,h^\dagger_{{\bf r}_2{\bf r}_1}\right )_{jj}
\left (h_{{\bf r}_1{\bf r}_4}\,h^\dagger_{{\bf r}_4{\bf r}_1} \right )_{jj},
\label{vertex}
\end{equation}
and the thick lines are the unperturbed propagator $\bar{C}^{-1}$. It turns out that the two-loop corrections cancel each other. This is a consequence of the anti-commuting property of the fermion field.
The details of the calculation are given in Appendix~\ref{app:details}.
Thus, in the Fourier space only the unperturbed propagator
\begin{equation}
{\tilde {\cal K}}_{\bf q} =\frac{1}{2-\int_{\bf k}
Tr_2 \left ({\tilde h}_{\bf k} \,{\tilde h}^\dagger_{{\bf k}-{\bf q}} \right )}
\label{diff_prop1}
\end{equation}
survives in this approximation. Here $\int_{\bf k}$ denotes the normalized integral with respect to the
$d$-dimensional sphere with radius $\lambda$.
The denominator of ${\tilde {\cal K}}_{\bf q}$ can be expanded in powers of ${\bf q}$. This leads to ${\tilde {\cal K}}_{\bf q}\sim 1/(A\,\epsilon+B\,q^2)$, provided the expansion exists and the system is isotropic. Due to the mirror-symmetric dispersion $(E_{\bf k},-E_{\bf k})$ of the PH-symmetric averaged Hamiltonian $H_0$,
we get
\begin{equation}
A=8\,\eta\int_{\bf k}\frac{1}{E_{\bf k}^2+\bar\eta^2}
\, ,\ \
B=\frac{1}{2}\int_{\bf k} Tr_2\left (\tilde{h}_{\bf k} \,\partial_{k_\mu}\partial_{k_\mu} \tilde{h}^\dagger_{\bf k} \right ) .
\label{diff_prop2}
\end{equation}
Thus, ${\tilde {\cal K}}_{\bf q}$ is a diffusion propagator with the diffusion coefficient $D=B/A$.
This perturbative result clearly indicates that diffusion is quite robust for a PH-symmetric Hamiltonian.
The robustness of diffusion in terms of a perturbation theory was also observed for the special case of 2d Dirac fermions \cite{PhysRevB.55.10661,PhysRevB.79.195424}.

\begin{figure}[t]
\begin{center}
\includegraphics[width=6.5cm,height=4cm]{feynman1}
\caption{\label{fig:feynman}
First order perturbation theory of ${\cal K}$ in Eq.~(\ref{prop2}) around the diffusion propagator $G$ for the (a) numerator,  and (b) the denominator. These terms cancel each other due to the symmetry of the blue square vertex.
}
\end{center}
\end{figure}

\section{Discussions}
\label{sect:discussion}

For a better understanding of the result in Eqs. (\ref{diff_prop1}) and (\ref{diff_prop2}),
we will consider a simple example of a two-band Hamiltonian. It is defined in the Fourier space with the dispersion $E_{\bf k}$ as
\begin{equation}
{\tilde h}_{\bf k}
=\sigma_0+\frac{2\,i\,\eta}{E_{\bf k}^2+\bar{\eta}^2}
\begin{pmatrix}
E_{\bf k}+i \,{\bar\eta} & 0 \\
0 & -E_{\bf k}+i\,{\bar\eta} \\
\end{pmatrix} ,
\end{equation}
which can also be written as
\begin{equation}
\tilde{h}_{\bf k}= \begin{pmatrix}
\kappa_{\bf k} & 0 \\
0 & \kappa_{\bf k}^*\\
\end{pmatrix} ,\ \ \
\kappa_{\bf k}=\frac{E_{\bf k}^2-\bar{\eta}^2
+2\,\epsilon\,\bar{\eta}+2 \,i\,\eta\, E_{\bf k}}{E_{\bf k}^2+\bar{\eta}^2} \,.
\end{equation}
In the limit $\epsilon\to0$, we get a unimodular function
\begin{equation}
\kappa_{\bf k}\to\frac{(E_{\bf k}+i\,\eta)^2}{E_{\bf k}^2+\eta^2}=e^{i\,\phi_{\bf k}}
\ , \ \
\phi_{\bf k}=\text{arg}\left [(E_{\bf k}^2+i\,\eta)^2) \right].
\label{unimodular1}
\end{equation}
The Fourier transform of $\bar{C}$ takes the form
\begin{equation}
\tilde{C}_{\bf q}=\int_{\bf k} \left [2-Tr_2
\left ({\tilde h}_{\bf k} \,{\tilde h}^\dagger_{{\bf k}-{\bf q}}\right ) \right ]
=\int_{\bf k} \left (2-\kappa_{\bf k}^*  \, \kappa_{{\bf k}-{\bf q}}
-\kappa_{\bf k}\, \kappa_{{\bf k}-{\bf q}}^*  \right ) ,
\label{int_C}
\end{equation}
which gives the expression $\tilde{C}_{\bf q}\sim A\epsilon+B\,q^2$ (as shown in Sec.~\ref{sect:fir}) for small ${\bf q}$. Here $A$ is defined as the integral in Eq.~(\ref{diff_prop2}) and
\begin{equation}
B=4\,\eta^2\int_{\bf k}
\frac{\left (\partial_{k_\mu} E_{\bf k} \right )\left (\partial_{k_\mu} E_{\bf k} \right )}
{\left (E_{\bf k}^2+\eta^2 \right )^2} \ .
\end{equation}
Our model has two independent parameters, the effective disorder strength $\eta$ and the momentum cut-off $\lambda$, where $1/\lambda$ defines the shortest wavelength. Moreover, the dimensionality $d$ of the ${\bf k}$-integration plays a crucial role. Although we do not expect that the qualitative behaviour of diffusion is much affected by the short-distance regime, the diffusion coefficient $D=B/A$ might depend on it.
In order to study this effect and its relation to different dispersions $E_{\bf k}$, we calculate it for two characteristic examples, namely $E_{\bf k}=E_s\, k^s$ with $s=1,2$. The expressions for $A$ and $B$
imply that the energy coefficient $E_s$ can be absorbed in the scaling of $\eta$ and $\epsilon$. Therefore, we implicitly assume subsequently that these parameters are scaled as $\eta\to\eta/E_s$ and $\epsilon\to\epsilon/E_s$.

The integral in Eq.~(\ref{int_C}) can be calculated for $\epsilon\sim0$, we obtain the results:
\begin{enumerate}
\item $E_{\bf k}=k$, $d=2$:
\begin{equation}
\tilde{C}_{\bf q}\sim \frac{4\,\eta} {3\,\lambda^4}
\left [
-\eta \,q^2+
6\,\eta^2\,\epsilon-3\,\eta\,\lambda^2+ 3\,\lambda^2
\left \lbrace
\frac{\eta  \left (q^2+2 \,\eta^2 \right )
\ln \left (1+ \frac {q\left (q+\sqrt{q^2+4 \,\eta^2} \right ) } {2 \,\eta^2} \right )}
{q \,\sqrt{4 \,\eta^2+q^2}}-4\,\epsilon  \ln(\eta/\lambda)
\right \rbrace \right ],
\end{equation}
and
\begin{equation}
\tilde{C}_{\bf q} \vert_{\mathbf q \sim 0}\sim\frac{4 \,\eta} {3\,\lambda}
\left [
\left \lbrace \frac{6 \,\eta^2} {\lambda^2}
-12\ln(\eta/\lambda)  \right \rbrace \frac{\epsilon}{\lambda} +
\frac{\lambda^2-\eta^2}{\eta} \,q^2
\right ].
\end{equation}

\item
$E_{\bf k}=k$, $d=3$:
\begin{equation}
\tilde{C}_{\bf q}\sim \frac{3\,\eta}{2\,\pi\,\lambda^3\,q}
\left [ \left (32\,\lambda\,\epsilon -2\,\pi\,\eta^2 \right ) q
+\pi\,\eta \left (4\,\eta^2+3\,q^2 \right )
{\rm arctan} \left ( \frac{q } {2\,\eta} \right )   \right ]
\end{equation}
and
\begin{equation}
\tilde{C}_{\bf q} \vert_{\mathbf q \sim 0}
\sim \frac{3\,\eta} {2\,\pi\,\lambda}
\left(\frac{32}{\lambda}\epsilon +\frac{4\pi}{3\,\lambda^2}q^2\right).
\end{equation}
This describes diffusion with a diffusion coefficient
$D=\lambda^2
\left ({\tilde\eta}^{-1}-{\tilde\eta} \right )/
\left (6\,{\tilde\eta}^2-12\ln {\tilde\eta} \right )$
with ${\tilde\eta}= \eta/\lambda$ in $d=2$ and
$D=\frac {\pi } {24  \,\lambda}$ in $d=3$.

\item
$E_{\bf k}=k^2$:
\begin{equation}
\tilde{C}_{\bf q}\sim
\begin{cases}
4 \, \lambda^{-2} \left [\epsilon  \left (\pi-2\eta/\lambda^2 \right )
+q^2/\lambda^2 \right ]
& \text{for } d=2\,, \\
\lambda^{-3}\sqrt{2\,\eta} \left (6\epsilon+\eta \,q^2 \right ) & \text{ for } d=3\,,
\end{cases}
\end{equation}
for $\epsilon\sim0$ and $q\sim0$.
This describes diffusion with diffusion coefficients $D=1/(\pi\lambda^2-2\, \eta)$ ($d=2$)
and $D=\eta/6$ ($d=3$). It is remarkable that $D$ vanishes with $\eta\to 0$ only in $d=3$,
but not in $d=2$.

\end{enumerate}

The results for the diffusion coefficients $D$ are summarized in Table \ref{table1}.
They clearly indicate that these diffusion coefficients depend strongly on the dispersion of $H_0$. A vanishing order parameter $\eta$ indicates a transition from the metallic phase to another phase, typically to an insulating phase. The results in Table \ref{table1} reveal that the properties of such a transition from the metallic side depend strongly on the details of the model and the dimensionality of the system. Although we focus on the metallic phase here, these properties might be interesting and deserve a further analysis to identify the strong influences of the PH-symmetric Hamiltonians.

\begin{table}
\begin{tabular}{| l | l | l |}
\hline
 & $d=2$ & $d=3$ \\ \hline
$E_{\bf k}=k$ &
$
\frac{\lambda^2\left ({\tilde\eta}^{-1}-{\tilde\eta} \right )}
{6 \, {\tilde\eta}^2-12  \ln \tilde \eta }$
& $\frac{\pi } {24\,\lambda} $\\
$E_{\bf k}=k^2$ &
$ \frac{1}
{\lambda^2  \left ( \pi-2\eta / \lambda^2 \right)} $
& $\eta/6$ \\
Dirac fermions & $-\frac{1}
{4\, \lambda \,{\tilde\eta} \ln{\tilde\eta} }$ & $-$ \\
\hline
\end{tabular}
\caption{The diffusion coefficients for the dispersions $E_{\bf k} $, and for dimensionalities $d=2,3$, with ${\tilde\eta}=\eta/\lambda$. The result for 2d Dirac fermions is from Ref.~\cite{PhysRevB.79.195424}.
}
\label{table1}
\end{table}

In conclusion, we have found that diffusion (i.e., metallic behaviour) is very robust if the
model Hamiltonian obeys the PH transformation property $H\to S\,H\,S^{-1}=-H$, as the one-loop and two-loop corrections vanish. The reason behind this is
the spontaneous PH symmetry-breaking, which is associated with a spontaneous breaking of a continuous symmetry, which creates a massless mode. However, the diffusion coefficient $D$ is very sensitive to the spectral properties of $H$ and the dimensionality of the underlying space. This connection between the underlying microscopic details of the model and the classical diffusion coefficient is an advantage of our approach, in comparison to more heuristic approaches (e.g., the Mori-Zwanzig memory matrix formalism \cite{Forster-HFBSCF,Freire-AP_2017,hartnoll2018holographic,ips-freire1,ips-freire2}). In particular, it will be interesting to apply this formalism to Luttinger semimetals, where methods like Kubo formula and memory matrix fail unless the PH symmetry is broken by unequal band masses \cite{rahul-sid,ips-rahul,ips-freire1,ips-freire2}. Finally, it will be worthwhile to see if our formalism can be used to compute transport properties in non-Fermi liquids having a critical Fermi surface \cite{ips-uv-ir1,ips-uv-ir2,ips-subir,ips-c2,ips-fflo,ips-nfl-u1}.

\section{Acknowledgments}
KZ gratefully acknowledges the support by the Julian Schwinger Foundation.

redpajama_set_name: RedPajamaArXiv


Stunning image matched by such beautiful prose.
Thanks Chris! Comes that day, and in this case night, when it's obvious the warmer weather is here to stay.
Interesting you should say this…I usually feel everything "surging" in one direction or another this time of year. This Spring seems to have a different quality. A suspended arrival….
Thanks! But the rain woke me up and I slid over in bed barely waking up to open the window to listen to it…. and it felt warm! An "awake" dream after the long winter!
yes, a lucid dream and a stream of consciousness.
That's so perfect John… it really could be the title! A gift? I'll use it….!!!!!
Where do we begin and where end in the unfurling into and out of whose voice whispering fingers sleeping spreading, fingers sleeping letters forming word word words like dew into mist like warm rain melting ice the window opening like your eyes… just barely.
Good to see you back Chris! I love it when you riff on something of mine. So much fun! Happy Spring…!


text:
RNA-polymeras är ett enzym som är direkt involverat i transkriptionen, det vill säga den process då cellens DNA omskrivs till budbärar-RNA (som sedan omskrivs till protein).

När en specifik gen ska transkriberas görs genens promotor tillgänglig så att RNA-polymeraset kan binda in. Det krävs även andra molekyler för att det ska kunna binda in på rätt ställe (till exempel olika transkriptionsfaktorer). Sedan vandrar RNA-polymeraset längs med genen, med cirka 20 nukleotider i sekunden, och styr tillverkningen av budbärar-RNA som är komplementärt till genen. När genen tagit slut lämnar RNA-polymeras genen och kan användas igen.

RNA-polymeras kan isoleras från celler för att sedan användas vid translationsförsök in vitro.

Se även
 RNA-polymeras II

Referenser

Enzymer

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text:
Walk-in COVID 19 testing now available on DTES
by Lisa Steacy
Posted Apr 22, 2020 1:24 pm PST
Last Updated Apr 22, 2020 at 1:25 pm PST
FILE: A healthcare worker prepares to collect a sample to test for COVID-19 at a drive-through testing site on March 20, 2020. THE ASSOCIATED PRESS/Wilfredo Lee
Walk-in testing is now available seven days a week at 611 Powell St.
The site offers testing to people with symptoms, and those connected to confirmed cases
Referral to COIVID-19 response centres, hotels, and housing is also offered
VANCOUVER (NEWS 1130) — A dedicated COVID-19 testing site has been set up on the Downtown Eastside.
Located at 611 Powell St., testing and referrals to housing and medical care will be available on a walk-in basis.
The centre will be open seven days a week from 9 a.m. to 4 p.m., and mobile testing is available to those who can't access the walk-in service.
Vancouver Coastal Health says the new site is meant to serve residents of the Downtown Eastside who are homeless, precariously housed, or otherwise vulnerable with symptoms including a cough, fever, or shortness of breath.
Anyone who has been in contact with someone who has tested positive is also eligible to be tested.
Takeout containers, bottled water needed for safe food distribution in DTESProvince working on solution to provide housing, increase support to homeless population: Dr. Bonnie HenryMuch more help needed on Vancouver's Downtown Eastside, say groups
coronavirus|COVDI-19|Downtown Eastside|testing|Vancouver Coastal Health

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text:
Q: Why is Pygame's KMOD_SHIFT unresolved and crashing my code? I wrote a simple program to test detection of the Shift key being pressed, I think it ought to work. The main issue seems to be the KMOD_SHIFT piece. I searched out shift detection using pygame and the test pygame.key.get_mods() & KMOD_SHIFT is what people said to use, and was in several code example as well. However, in MY code I get a warning that KMOD_SHIFT is an unresolved reference, and when I try to run the code, as soon as I press any key I get an error: "name KMOD_SHIFT is undefined".
Isn't Pygame supposed to define it? In other people's code examples of using this, they seem to be using it the same as me. What am I doing wrong here?
Still a major Python newbie - thanks for your guidance.
#! /usr/bin/python3

import pygame

pygame.init()
screen_width, screen_height = 800, 600
screen_color = [128, 128, 128]

game_display = pygame.display.set_mode((screen_width, screen_height))
pygame.display.set_caption('Coloriffic')
clock = pygame.time.Clock()

my_font = pygame.font.SysFont("monospace", 45)

crashed = False
shift_label = my_font.render("shift is NOT pressed", 1, (0, 0, 0))

while not crashed:
    for event in pygame.event.get():
        if event.type == pygame.QUIT:
            crashed = True
        if event.type == pygame.KEYDOWN:
            if pygame.key.get_mods() & KMOD_SHIFT: # the problem line
                shift_label = my_font.render("shift is pressed", 1, (0, 0, 0))
            else:
                shift_label = my_font.render("shift is NOT pressed", 1, (0, 0, 0))

    game_display.fill(screen_color)
    game_display.blit(shift_label, (100, 100))

    pygame.display.update()
    clock.tick(60)

pygame.quit()
quit()

A: Nevermind, it seems that if I use pygame.KMOD_SHIFT all works fine. I don't know why other people didn't have to put the "pygame." in front, maybe they imported Pygame differently than I did.
False alarm, my apologies.

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text:
You are here: Home / Fires/Accidents/Disasters / Heavy winds caused concern with Clearfield egg facility fire
Heavy winds caused concern with Clearfield egg facility fire
November 29, 2021 By Dar Danielson
Clearfield egg plant fire. (KMA photo)
Clearfield Mayor Chris Knox is hoping an egg production facility that was heavily damaged by fire this weekend will be able to recover.
Knox says he noticed the plant burning at around 7:30 Saturday morning — and most of the facility's employees were standing outside when he drove by. The mayor says the gusty winds made for what he called "a scary deal."
"The wind did pick up pretty strong there Saturday afternoon," he says. "It was blowing right towards town at that particular time, and there was a pretty big concern about starting a cornfield on fire right to the east side of where the fire was. From there, it could have carried into the town of Clearfield."
Knox says the facility was bought from Iowa Cage-Free last month and is now known as Hen Haven Fire crews brought the fire under control by about 6 p-m Saturday–but not before it caused considerable damage.
"One complete hen house was burned clear to the ground. I would estimate it to be 700-to-800 feet long. It took it completely down. From there, the barn was connected by breezeways to the processing facility, and to the office space, and I believe to the distribution center. The processing, the office space, and the distribution area were all completely damaged, as well," according to Knox.
It's believed hundreds of thousands of chickens died in the fire. Know says the plant employs up to 70 people and the fire is a big blow to more than just the facility's workers.
"It goes to people supplying the facility with feed resources and other resources," he says. "It doesn't even affect just the employees, it affects everybody that has ties to that business, as well. It would be really great if we could salvage what we can out of the mess, and continue to have that for the community. It really would."
Knox praised fire departments from surrounding communities for their assistance in battling the fire. There's no word on what caused the fire. None of the facility's employees were injured, but Knox says two firefighters reportedly were treated for smoke inhalation.
(By Mike Peterson, KMA, Shenandoah)
Filed Under: Agriculture, Fires/Accidents/Disasters, News


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— Few hours
405 miles / 6h 30min
Denver (DEN) — Rapid City (RAP)
617 miles / 12h
Rapid City (RAP) — Dickinson (DIK)
Dickinson (DIK) — Medora
658 miles / 12h 15min
Rapid City — Glendive, MT
Glendive, MT — Medora
63 miles / 1h 5min
Medora — Dickinson (DIK)
Dickinson (DIK) — Bozeman (BZN)
Medora — Glendive, MT
Glendive, MT — West Yellowstone, MT
West Yellowstone, MT — West Yellowstone
0 miles / 9min
West Yellowstone — Bozeman
89 miles / 2h 15min
161 miles / 4h
Bozeman — Gardiner
Gardiner — Yellowstone National Park
Drive + Fly: 3h 30min
Yellowstone National Park — Jackson (JAC)
Jackson (JAC) — Salt Lake City (SLC)
Fastest: 1h 5min
Yellowstone National Park — Grand Targhee Resort
Grand Targhee Resort — Idaho Falls (IDA)
Idaho Falls (IDA) — Salt Lake City (SLC)
Salt Lake City (SLC) — Twin Falls (TWF)
Fastest: 2h 45min(flight time: 56min)
Fly + Taxi: 5h 15min
Twin Falls (TWF) — Kalispell (FCA)
Kalispell (FCA) — Glacier National Park
Twin Falls — Spokane Amtrak Station
Spokane Amtrak Station — West Glacier Amtrak
Glacier National Park — Kalispell (FCA)
Kalispell (FCA) — Denver (DEN)
1192 miles / 28h
Glacier National Park — East Glacier Park Amtrak
East Glacier Park Amtrak — Shelby Amtrak
Shelby Amtrak — Great Falls, MT
Great Falls, MT — Butte, MT
Butte, MT — Denver
Denver (DEN) — Atlanta (ATL)
Denver — Colorado Springs, CO
Colorado Springs, CO — Colorado Springs (COS)
Colorado Springs (COS) — Atlanta (ATL)
End: Atlanta
Read more about United States
Destinations in United States
Things to do in United States
Mile-High City
Aptly nicknamed the "Mile-High City," Denver sits at an altitude of 1,600 m (5,280 ft) above sea level, located right where the Great Plains give way to the Rocky Mountains.
To see traveler tips, reviews, where to stay, and tourist information, refer to the Denver online trip maker .
Atlanta to Denver is an approximately 5.5-hour flight. You can also do a combination of flight and bus; or drive. Traveling from Atlanta to Denver, you'll gain 2 hours due to the time zone difference. Traveling from Atlanta in June, plan for a bit cooler nights in Denver, with lows around 55°F. You will leave for Rapid City on the 28th (Sun).
Outdoors Parks Tours
Gateway to the Black Hills
South Dakota's second-largest city, Rapid City has for many years served as a gateway to the West.
On the 29th (Mon), make a trip to Dinosaur Park, wander the streets of Downtown Rapid City, and then stroll the grounds of Mount Moriah Cemetery. Get ready for a full day of sightseeing on the 30th (Tue): explore the striking landscape of Mount Rushmore National Memorial.
To find where to stay, more things to do, reviews, and more tourist information, read Rapid City online tour planner .
Getting from Denver to Rapid City by flight takes about 3.5 hours. Other options: drive; or take a bus. Traveling from Denver in June, expect nights in Rapid City to be about the same, around 57°F, while days are little chillier, around 78°F. Wrap up your sightseeing by early afternoon on the 30th (Tue) to allow enough time to drive to Medora.
Things to do in Rapid City
Parks Nature Historic Sites
Mount Moriah Cemetery, Mount Rushmore National Memorial
Mount Moriah Cemetery
9:30am, Mon Jun 29
Medora is a city in Billings County, North Dakota, United States. Kick off your visit on the 1st (Wed): get to know the fascinating history of Painted Canyon Overlook and then appreciate the extensive heritage of South Unit.
For other places to visit, more things to do, where to stay, and other tourist information, you can read our Medora route tool .
Drive from Rapid City to Medora in 4.5 hours. Alternatively, you can do a combination of flight and taxi; or do a combination of bus and taxi. Expect little chillier evenings in Medora when traveling from Rapid City in June, with lows around 50°F. Finish up your sightseeing early on the 1st (Wed) so you can travel to Bozeman.
Things to do in Medora
Historic Sites Parks Nature
South Unit
12:00pm, Wed Jul 1
Painted Canyon Overlook
10:00am, Wed Jul 1
Bozeman is a city in and the county seat of Gallatin County, Montana, United States, in the southwestern part of the state. To plan Bozeman vacation without wasting time, ask Inspirock to design an itinerary.
You can do a combination of taxi and flight from Medora to Bozeman in 5.5 hours. Alternatively, you can drive; or do a combination of car and bus. Expect little chillier evenings in Bozeman when traveling from Medora in July, with lows around 50°F. You will leave for Yellowstone National Park on the 2nd (Thu).
Things to do in Bozeman
Outdoors Tours Parks
World's Largest Collection of Geysers
An exceptionally diverse landscape and varied wildlife have made Yellowstone National Park one of America's most popular parks.
Get ready for a full day of sightseeing on the next day: take in breathtaking views at Grand Canyon of the Yellowstone, hike along Artist Point, witness a stunning natural landmark at Old Faithful, then witness a stunning natural landmark at Grand Prismatic Spring, and finally witness a stunning natural landmark at Mammoth Hot Springs.
For more things to do, reviews, maps, and other tourist information, read Yellowstone National Park online trip itinerary planner .
Traveling by car from Bozeman to Yellowstone National Park takes 3.5 hours. Alternatively, you can do a combination of bus and car; or take a bus. Expect little chillier temperatures when traveling from Bozeman in July; daily highs in Yellowstone National Park reach 73°F and lows reach 39°F. Wrap up your sightseeing on the 4th (Sat) to allow time to travel to Salt Lake City.
Things to do in Yellowstone National Park
Parks Nature Wildlife
Grand Canyon of the Yellowstone
9:00am, Fri Jul 3
9:30am, Sat Jul 4
1:00pm, Fri Jul 3
Crossroads of the West
Utah's capital and most populous city, Salt Lake City boasts a small-town feel, big-city amenities, and plenty of nature on its doorstep.
Get some historical perspective at Temple Square and Salt Lake Temple.
For more things to do, reviews, other places to visit, and tourist information, refer to the Salt Lake City driving holiday planner.
Getting from Yellowstone National Park to Salt Lake City by combination of car and flight takes about 3.5 hours. Other options: drive; or do a combination of car, shuttle, and flight. Traveling from Yellowstone National Park in July, things will get much warmer in Salt Lake City: highs are around 95°F and lows about 70°F. On the 7th (Tue), you'll travel to Twin Falls.
Historic Sites Parks
Temple Square
4:30pm, Mon Jul 6
Salt Lake Temple
Twin Falls is the county seat and largest city of Twin Falls County, Idaho, United States. For more things to do, ratings, maps, and tourist information, you can read our Twin Falls travel itinerary planner .
You can fly from Salt Lake City to Twin Falls in 3 hours. Other options are to drive; or take a bus. Expect a bit cooler evenings in Twin Falls when traveling from Salt Lake City in July, with lows around 61°F. You'll set off for Glacier National Park on the 9th (Thu).
Things to do in Twin Falls
Parks Nature Outdoors
Crown of the Continent
The glaciers from which Glacier National Park takes its name mostly dissipated eons ago, but they left behind a scoured landscape of high and steep mountain peaks, sparkling lakes, lush alpine meadows, and thick forests.
Start off your visit on the 9th (Thu): explore the striking landscape at Jackson Glacier Overlook. On the next day, admire the verdant scenery at Logan Pass, then stroll through Highline Trail, and then stroll through Grinnell Glacier.
To see traveler tips, other places to visit, photos, and tourist information, refer to the Glacier National Park itinerary planning tool .
Getting from Twin Falls to Glacier National Park by combination of flight and taxi takes about 5.5 hours. Other options: drive; or do a combination of bus and train. Expect slightly colder temperatures when traveling from Twin Falls in July; daily highs in Glacier National Park reach 85°F and lows reach 49°F. Wrap up your sightseeing by early afternoon on the 12th (Sun) to allow time for travel to Denver.
Things to do in Glacier National Park
3:30pm, Fri Jul 10
10:00am, Sat Jul 11
For reviews, ratings, other places to visit, and other tourist information, use the Denver online sightseeing planner .
Traveling by combination of taxi and flight from Glacier National Park to Denver takes 5.5 hours. Alternatively, you can drive; or do a combination of car, train, bus, and shuttle. Traveling from Glacier National Park in July, Denver is somewhat warmer at night with lows of 60°F. On the 13th (Mon), you'll travel back home.
19 days in Seattle & Yellowstone National Park BY A USER FROM UNITED STATES August, outdoors, relaxing, beaches, museums, wildlife, popular & hidden gems PREFERENCES: August, outdoors, relaxing, beaches, museums, wildlife ATTRACTION STYLE: Popular & hidden gems PACE: Medium 20 days in United States BY A USER FROM UNITED STATES June, teens, kids, culture, outdoors, historic sites, museums, wildlife, popular & hidden gems PREFERENCES: June, teens, kids, culture, outdoors, historic sites, museums, wildlife ATTRACTION STYLE: Popular & hidden gems PACE: Medium 19 days in United States BY A USER FROM UNITED STATES August, culture, outdoors, wildlife, slow & easy, popular & hidden gems PREFERENCES: August, culture, outdoors, wildlife ATTRACTION STYLE: Popular & hidden gems PACE: Slow & easy 18 days in United States BY A USER FROM UNITED STATES September, outdoors, relaxing, historic sites, museums, wildlife, popular sights PREFERENCES: September, outdoors, relaxing, historic sites, museums, wildlife ATTRACTION STYLE: Popular sights PACE: Medium 23 days in United States BY A USER FROM UNITED STATES August, culture, outdoors, relaxing, beaches, historic sites, museums, shopping, wildlife, slow & easy, popular sights PREFERENCES: August, culture, outdoors, relaxing, beaches, historic sites, museums, shopping, wildlife ATTRACTION STYLE: Popular sights PACE: Slow & easy 22 days in Yellowstone National Park BY A USER FROM UNITED STATES September, kids, culture, outdoors, relaxing, beaches, historic sites, museums, shopping, wildlife, slow & easy, popular & hidden gems PREFERENCES: September, kids, culture, outdoors, relaxing, beaches, historic sites, museums, shopping, wildlife ATTRACTION STYLE: Popular & hidden gems PACE: Slow & easy 33 days in United States BY A USER FROM AUSTRALIA October, culture, outdoors, relaxing, beaches, historic sites, museums, shopping, wildlife, hidden gems PREFERENCES: October, culture, outdoors, relaxing, beaches, historic sites, museums, shopping, wildlife ATTRACTION STYLE: Hidden gems PACE: Medium 17 days in United States BY A USER FROM UNITED STATES September, culture, outdoors, historic sites, wildlife, popular & hidden gems PREFERENCES: September, culture, outdoors, historic sites, wildlife ATTRACTION STYLE: Popular & hidden gems PACE: Medium 23 days in United States BY A USER FROM SPAIN August, culture, outdoors, relaxing, romantic, historic sites, museums, shopping, wildlife, popular sights PREFERENCES: August, culture, outdoors, relaxing, romantic, historic sites, museums, shopping, wildlife ATTRACTION STYLE: Popular sights PACE: Medium 19 days in United States BY A USER FROM UNITED STATES June, teens, culture, outdoors, historic sites, wildlife, popular sights PREFERENCES: June, teens, culture, outdoors, historic sites, wildlife ATTRACTION STYLE: Popular sights PACE: Medium
Yellowstone National Park trip planner
Best things to do in Twin Falls
Best things to do in Glacier National Park
The Best Nature Reserves in South Dakota


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Workshop Seat
Book (The Geography of Friendship)
Pick up book at event
Crafting Words - Sally Piper: Witnessing Landscape
In store at Avid Reader Bookshop
Workshop Seat $75.00, Book (The Geography of Friendship) $29.95
Tickets available until 05 July 2020 12:00 PM
Join Sally Piper, author of The Geography of Friendship as she takes us on a deep dive into the relationship between humans and the natural world in this three hour Crafting Words Workshop, Witnessing Landscape: Writing the human connections to landscape.
This is more than a nature-writing workhshop, this is an exploration of the threads and connections that inextricably link human kind with the natural world and how to capture and honour these connections in your writing.
Sally Piper is a Brisbane-based writer of novels, short fiction and non-fiction. She is a former nurse and nurse educator, specialising in neurosurgical critical care, and has worked in both Australia and the UK. Her long nursing career taught her much about the vulnerabilities of people, but also the fortitude of those faced with extreme adversity. It is a career that continues to inform her writing, most notably when developing strengths, flaws and frailties in her characters.
Her debut novel Grace's Table (UQP 2014/Legend Press UK 2019) was shortlisted for the 2011 Queensland Premier's Literary Award - Emerging Queensland Author category and in 2013 she was awarded a Varuna Publishing Fellowship for her manuscript. Her second novel The Geography of Friendship (UQP 2018/Audible Audiobooks/Legend Press UK 2019) was shortlisted for the 2019 Australian Book Industry Awards - Small Publishers' Adult Book of the Year category and selected as an Australian Women's Weekly Great Read.
Her short fiction and non-fiction has appeared in various online and print publications in Australia and the UK, to include a prize-winning short story in an anthology, Griffith Review, The Saturday Paper, The Sydney Morning Herald, The Weekend Australian and other literary magazines and journals. She has been interviewed for radio, been a guest panellist at literary festivals and delivered many author talks and readings.
Sally holds a Master of Arts (Research) in Creative Writing from Queensland University of Technology. During her post-graduate studies she also tutored on the QUT Creative Writing program. She is an active member of the Queensland writing community, where she presents workshops and seminars, leads in-conversations and mentors other writers.
She is a self-confessed nature nerd and likes nothing more than long bush walks to escape her desk.
SEE MORE CRAFTING WORDS WORKSHOPS HERE


This Delightful Eternity ring has been hand set with a beautiful number of 2.5mm round Sapphires & Pearls. A beautifully designed eternity / band style ring, which can easily be worn at the same finger as an existing wedding ring (being 4mm wide) and the stones are set very securely with the setting being safe by the quite raised edge.
These are Genuine Natural Sapphires & Pearls.
The Silver is Solid Sterling Silver authenticated by the Assay Place of business in London, England. They have got stamped their mark at the inside of the shank to confirm that this ring is made of Solid 925 Sterling Silver. This mark is unique to the Assay Place of business in London and will only be found on High Quality Silver articles.
This ring used to be Designed and Made in England, and can be sent to you in a Luxury Presentation ring box.


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Listening Bar
See the Sunrise Skyline at Boulton and TJ Finley's
Music lisa heffernan | August 13, 2010
Their music has been described as the love child of the Black Crowes and the Counting Crows, but Sunrise Skyline has an eclectic sound which can be heard on their latest full-length, "Hey Friend…" The LI natives have been together for nearly three years, and rhythm guitarist Nick Petrillo says their name reflects their roots—"as the sunrise comes from the east, and the skyline of the city is to the west."
Influenced by Pearl Jam and the Dave Matthews Band, the quintet also includes Anthony Pravata on lead guitar, Rob Caniglia on drums, Ken Cavallero on bass, and the Caleb Followill-esque sounding lead vocalist, Jon March. The band's 11-track disc was recorded locally at On Track Recording Studios, and includes rockers like "High" and "Us," along with some more melancholic songs like "Sunrise" and the cello-laden stand-out track, "Gone," featuring Jon Preddice from local acoustic-folk-rock band Miles to Dayton on the cello.
Known for their captivating live performances, Sunrise Skyline is excited to play a sold-out show at the YMCA Boulton Center for the Performing Arts on Saturday, August, 14th, for their CD release party. If you don't have a ticket to the Boulton, you can still head across the street for the after party at TJ Finley's, where CD's will be available for $10. And if you're interested in the top shelf open bar from 10:30pm-1:30am, there will be a $35 cover at the door. So get ready to sit back and enjoy the Sunrise, because Petrillo says they're ready to put LI bands and music back in the forefront: "The goal is to have someone be able to put our album on at a back yard party and just let it play all the way through and keep the mood flowing." For more info check out: http://www.sunriseskyline.com
lisa heffernan
Lisa Heffernan received a master's in Communications from Emerson College before moving to New York. She has worked for publications such as: Details, Nylon, Rolling Stone, Time Out, Newport Mercury, American Songwriter and W magazine.
Glenn Hughes Revisits Deep Purple
Giving fans what they want
He-Bird, She-Bird's Musical Ascent
Americana at its best


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Animals Australia Unleashed
Animals Australia Unleashed is the youth outreach division of Animals Australia, Australia's largest and most dynamic animal protection organisation. Animals Australia campaigns to protect all animals, and is known for its groundbreaking work in investigating and exposing animal cruelty.
Barefoot Vegan
Situated in the beautiful, lush green of the south-west of France, the Barefoot Vegan Farm and Sanctuary is a space of learning, teaching, healing and loving for humans and animals.
Cruelty Free International is the leading organisation working to end animal experiments worldwide. They work to end animal experiments by investigating and exposing the reality of life for animals in laboratories, challenging decision-makers to make a positive difference for animals, and championing better science and cruelty free living.
PETA is the largest animal rights organisation in the world, with more than 5 million members and supporters. PETA focuses its attention on the four areas in which the largest numbers of animals suffer the most intensely for the longest periods of time: on factory farms, in the clothing trade, in laboratories, and in the entertainment industry.
Royal Society for Prevention Cruelty to Animals (RSPCA)
The RSPCA is an Australian independent, non-government community-based charity providing animal care and protection services. The RSPCA runs 40 shelters and employs around 1,000 staff. It costs more than $100 million each year to deliver all of their services which help improve the lives of Australian animals.


Everyone loves mac and cheese, but sometimes you want to make something for dinner that has a little kick. My Spicy Mac And Cheese is a great twist on a classic! You can control the amount of spice by only using one of the chipotle peppers (or three if you want it spicier!) or not using jalapeno slices at all. Try to tailor it to what you think will work best for your family. A perfect way to celebrate Cinco de Mayo or just time with friends and family!
Preheat your oven to 400 degrees. In a large pot, boil water and cook the macaroni until al dente, about 7 minutes. While the pasta is cooking, take out your blender. Add the milk, garlic powder, oregano, pepper and chipotle peppers and blend until the chipotles are finely chopped.
Once ready, drain the macaroni and set it aside in a colander. Return the pot to low heat and melt the butter. Add the flour and cook for one minute.
Increase the heat to medium and slowly whisk in the milk mixture. Keep whisking until it comes to a simmer and thickens.
Add the Colby Jack cheese a handful at a time, whisking until completely melted between each addition. Add the Velveeta and whisk until melted. Remove your pot from the heat and add the drained macaroni. Stir to combine.
Pour the now cheesy pasta into a lightly greased 13×9 baking dish. Bake until it just starts to brown, about 15-20 minutes. Serve hot with jalapeno slices.
In a large pot, boil water and cook macaroni until al dente, about 7 minutes.
While the pasta is cooking, take out your blender.
Add milk, garlic powder, oregano, pepper and chipotle peppers and blend until the chipotles are finely chopped.
Once ready, drain the macaroni and set it aside in a colander.
Return the pot to low heat and melt the butter.
Add the flour and cook for one minute.
Increase the heat to medium and slowly whisk in the milk mixture.
Keep whisking until it comes to a simmer and thickens.
Add Colby Jack cheese a handful at a time, whisking until completely melted between each addition.
Add Velveeta and whisk until melted.
Remove your pot from the heat and add the drained macaroni.
Pour the pasta into a lightly greased 13x9 baking dish.
Bake until it just starts to brown, about 15-20 minutes.
Serve hot with jalapeno slices.
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We had a surprise visit today from two very special guests.....find out who here!
Today started just like any other day. The children woke up, we all lined up quietly and went down to breakfast as normal. However..........little did we know that Mrs Monahan and Mrs Redmond were on their way down to visit us on the train to Portsmouth where they the boarded a ferry to the Isle of Wight! (Dun dun dunnn! I hear you cry!).
As we lined up for our first activities of the day, the children suddenly saw a very familiar pair of faces coming towards them and all let out screams of excitement! Everyone was in shock, including us teachers who had no idea at all!
Mrs Monahan and Mrs Redmond joined us on a couple of activities followed by a whistle stop tour of the camp and some much needed lunch in the canteen. They then joined Miss Scannells group on the Culver walk before leaving to return back to school.
This afternoon the children were all allowed to visit the tuck shop where they could spend their pocket money on whatever they wanted. The lure of sweets did sway a few, but other Children including myself bought some litte Isle of Wight nic-nacs for their loved ones.
All groups then split into their activities for the day. This included Team Tech where the children were split into teams of two in a Dragons Den style event. Each team was given a bag of mystery objects that the children then had to build into a product, this was then judged by the teacher and instructor. In one of the groups the first team created a scooter that could be folded down making it easy to transport. This came with some accessories that could also be used to bling up the scooters.
The second team made a doggie transporter designed to aid dogs with disabilities or who were unable to easily walk. This came with some doggie toys the children designed with the remaining objects.
Both projects were really creative as all the children worked very cooperatively together! After much deliberation between the judges, they decided to make team two the winners, we could like to offer our congratulations to all involved!
Another activity a couple of the groups took part in was nightline. In this activity the children had to make their way through a sensory trail whilst blind folded and holding the waist of the camp mate in front of them. The children found this highly amusing as they had to negotiate their way through some very tricky obstacles whilst the instructors and teachers messed around with them by spraying water and tapping their arms with leaves and branches as they went though each obstacle. It was honestly hilarious and the children thoroughly enjoyed it!
After another busy day of activities we then sat down to a lovely roast dinner and some teriyaki pork before returning to our lodges for a bit of free time and some hot cocoa. We are now getting ready for bed and an exciting day on the beach tomorrow! Tune in for more fun and excitement then!
Photos can be seen in our day three gallery by CLICKING HERE!