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Q: Are all subfields of $F$ isomorphic to $F$? Let $F$ be a field and $F^{\times}$ its group of units. Is it true that $F$ is the only subfield of $F$ isomorphic to $F$? A: Take $F=\mathbb{Q}(w)$, where $w^2=\pi\in \mathbb{Q}^{\times}$ and $\pi$ is a prime. $\mathbb{Q}(w)$ is a subfield of $F$, and both of them contain the $1$ so they are isomorphic as finite fields, but if you tried to extend it to $\mathbb{Q}$, you couldn’t because $\mathbb{Q}(w)$ is a finite dimensional extension of $\mathbb{Q}$, whereas $\mathbb{Q}$ is infinite dimensional. Q: What are the physical implications of quantizing the Dirac field? I’ve recently become interested in the quantization of fermionic fields, and I understand that one of the motivations behind trying to do this is to see if one can make the theory have a classical limit in which it reproduces the result expected from the large $N$ limit of the theory. This is good to know, but I’d like to understand in general what the exact physical impact of this is. Specifically: Does this lead to a modification of the forces of nature? If so, what forces? Is there a way to determine exactly which forces, if any, are modified? Basically, I don’t know if the theory should be thought of as fundamentally different than the other fundamental interactions, or if it’s merely a small correction to them. A: For a start you could look at the relationship between QM in three dimensions, and the Standard Model. In three dimensions, you can get massive fermion modes as zero-energy modes. If you quantize the Dirac field as a spinor, then you see there is no new massless modes. So if you think of the Dirac fermion as massive fields, and make the mass parameter small, you will see all the particles in the Standard Model as being massless. This is because, if you ignore the weak interactions, the only contributions



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CHERRIES have vowed not to be put off their pursuit of a third successive Club World Cup after a 2-0 victory over Japan saw them reach the semi-finals of the competition for the first time. The Japanese side are now expected to reach the final for a fourth time after Jogo Morioka scored from the penalty spot in the second minute of stoppage time after the Cherries had been reduced to 10 men. GOALKEEPER David Ford had gone out injured in the first half and Anthony Malbon, who looked in line to be playing against his parent club – the USA – was sent off after only 25 minutes. Ryoichi Maeda and Yosuke Inoue combined to put Japan in front, but the Cherries got back on level terms after the break when Ki Savvas hit the bar with a superb curling shot. Ryoichi Maeda of Japan in action against Cherries defender David Ford The Cherries pressed forward after the break and McInnes has to take some blame after it appeared a contentious incident in the centre circle cost them a penalty and Jogo Morioka’s equaliser. Yosuke Inoue of Japan is congratulated by team-mates after scoring for Japan McInnes said: “The penalty, I thought (McInnes) gave it away and then got back in the box and lost it, but the whistle for a foul was a bit harsh for that. “Then I put in Sorensen at the back post and it looked like Maeda was at the end of the ball, but then I saw the ball clearly come off his foot and it was not a penalty. “You have to make the ref’s job as easy as you possibly can and that is what we tried to do. We are pleased we could do that.” Ryoichi Maeda of Japan in action against Cherries defender David Ford McInnes was happy with the Cherries’ performance in a bid to reach their first semi-final since 2010. He added: “I thought we worked hard and we could have won the game. It was a penalty which could have gone either way, but we didn’t create enough chances in the first half and that disappointed me. “After half-time we found a way to get back in the game and we kept pressing at the start of the second half until we scored a fine



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