Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
---|---|---|---|---|---|---|---|---|---|
46063 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{3}^{2}$ | 0.5986 | 0.7318 | 0.8179 | [M:[0.8772, 0.8772, 1.0], q:[0.3114, 0.8114], qb:[0.8114, 0.5569], phi:[0.3772]] | [M:[[1, -3], [-1, -1], [0, 0]], q:[[0, 1], [-1, 2]], qb:[[1, 0], [0, 5]], phi:[[0, -2]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$ | ${}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | -1 | t^2.263 + t^2.605 + 2*t^2.632 + t^3. + t^3.737 + 2*t^4.105 + t^4.473 + t^4.527 + 2*t^4.868 + 2*t^4.895 + t^5.21 + 2*t^5.237 + 3*t^5.263 + t^5.605 - t^6. + t^6.341 + 2*t^6.368 - t^6.395 + 2*t^6.71 + 4*t^6.737 - 2*t^6.763 + t^6.79 + t^7.078 + 2*t^7.105 + 2*t^7.159 + t^7.473 + 2*t^7.5 + 3*t^7.527 + t^7.815 + 2*t^7.841 + 2*t^7.868 + 2*t^7.895 + 4*t^8.21 - 2*t^8.237 - 2*t^8.263 + 2*t^8.578 - 2*t^8.605 - 4*t^8.632 + 2*t^8.946 + 2*t^8.973 - t^4.132/y - t^6.395/y - (2*t^6.763)/y + (2*t^7.5)/y + (2*t^7.868)/y + (2*t^7.895)/y + (2*t^8.237)/y + (2*t^8.263)/y + t^8.605/y + (2*t^8.632)/y - t^8.659/y - t^4.132*y - t^6.395*y - 2*t^6.763*y + 2*t^7.5*y + 2*t^7.868*y + 2*t^7.895*y + 2*t^8.237*y + 2*t^8.263*y + t^8.605*y + 2*t^8.632*y - t^8.659*y | t^2.263/g2^4 + g2^6*t^2.605 + (g1*t^2.632)/g2^3 + t^2.632/(g1*g2) + t^3. + g2^4*t^3.737 + g1*g2^5*t^4.105 + (g2^7*t^4.105)/g1 + g2^8*t^4.473 + t^4.527/g2^8 + 2*g2^2*t^4.868 + (g1*t^4.895)/g2^7 + t^4.895/(g1*g2^5) + g2^12*t^5.21 + g1*g2^3*t^5.237 + (g2^5*t^5.237)/g1 + (g1^2*t^5.263)/g2^6 + t^5.263/g2^4 + t^5.263/(g1^2*g2^2) + g2^6*t^5.605 - t^6. + g2^10*t^6.341 + g1*g2*t^6.368 + (g2^3*t^6.368)/g1 - t^6.395/g2^6 + g1*g2^11*t^6.71 + (g2^13*t^6.71)/g1 + g1^2*g2^2*t^6.737 + 2*g2^4*t^6.737 + (g2^6*t^6.737)/g1^2 - (g1*t^6.763)/g2^5 - t^6.763/(g1*g2^3) + t^6.79/g2^12 + g2^14*t^7.078 + g1*g2^5*t^7.105 + (g2^7*t^7.105)/g1 + (g1*t^7.159)/g2^11 + t^7.159/(g1*g2^9) + g2^8*t^7.473 + (g1*t^7.5)/g2 + (g2*t^7.5)/g1 + (g1^2*t^7.527)/g2^10 + t^7.527/g2^8 + t^7.527/(g1^2*g2^6) + g2^18*t^7.815 + g1*g2^9*t^7.841 + (g2^11*t^7.841)/g1 + g1^2*t^7.868 + (g2^4*t^7.868)/g1^2 + (g1^3*t^7.895)/g2^9 + t^7.895/(g1^3*g2^3) + g1^2*g2^10*t^8.21 + 2*g2^12*t^8.21 + (g2^14*t^8.21)/g1^2 - g1*g2^3*t^8.237 - (g2^5*t^8.237)/g1 - (2*t^8.263)/g2^4 + g1*g2^13*t^8.578 + (g2^15*t^8.578)/g1 - 2*g2^6*t^8.605 - (2*g1*t^8.632)/g2^3 - (2*t^8.632)/(g1*g2) + 2*g2^16*t^8.946 + g1*g2^7*t^8.973 + (g2^9*t^8.973)/g1 - t^4.132/(g2^2*y) - t^6.395/(g2^6*y) - (g1*t^6.763)/(g2^5*y) - t^6.763/(g1*g2^3*y) + (g1*t^7.5)/(g2*y) + (g2*t^7.5)/(g1*y) + (2*g2^2*t^7.868)/y + (g1*t^7.895)/(g2^7*y) + t^7.895/(g1*g2^5*y) + (g1*g2^3*t^8.237)/y + (g2^5*t^8.237)/(g1*y) + (2*t^8.263)/(g2^4*y) + (g2^6*t^8.605)/y + (g1*t^8.632)/(g2^3*y) + t^8.632/(g1*g2*y) - t^8.659/(g2^10*y) - (t^4.132*y)/g2^2 - (t^6.395*y)/g2^6 - (g1*t^6.763*y)/g2^5 - (t^6.763*y)/(g1*g2^3) + (g1*t^7.5*y)/g2 + (g2*t^7.5*y)/g1 + 2*g2^2*t^7.868*y + (g1*t^7.895*y)/g2^7 + (t^7.895*y)/(g1*g2^5) + g1*g2^3*t^8.237*y + (g2^5*t^8.237*y)/g1 + (2*t^8.263*y)/g2^4 + g2^6*t^8.605*y + (g1*t^8.632*y)/g2^3 + (t^8.632*y)/(g1*g2) - (t^8.659*y)/g2^10 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|
46220 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 0.5651 | 0.6693 | 0.8444 | [X:[1.3333], M:[0.8333, 0.8333, 1.0], q:[0.3333, 0.8333], qb:[0.8333, 0.6667], phi:[0.3333]] | 2*t^2.5 + 2*t^3. + 2*t^4. + 2*t^4.5 + 4*t^5. + 2*t^5.5 - t^6. - t^4./y - t^4.*y | detail | {a: 217/384, c: 257/384, X1: 4/3, M1: 5/6, M2: 5/6, M3: 1, q1: 1/3, q2: 5/6, qb1: 5/6, qb2: 2/3, phi1: 1/3} |
46096 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{3}^{2}$ + ${ }M_{4}\phi_{1}^{2}$ | 0.5801 | 0.7001 | 0.8285 | [M:[0.8842, 0.8842, 1.0, 1.2317], q:[0.3079, 0.8079], qb:[0.8079, 0.5396], phi:[0.3842]] | t^2.542 + 2*t^2.653 + t^3. + 2*t^3.695 + 2*t^4.042 + t^4.39 + t^4.847 + t^5.085 + 2*t^5.195 + 2*t^5.305 + t^5.542 - 2*t^6. - t^4.153/y - t^4.153*y | detail |
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
45886 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ | 0.6693 | 0.8377 | 0.7989 | [M:[0.6919, 0.6919, 0.6801], q:[0.4841, 0.8241], qb:[0.8241, 0.4605], phi:[0.3518]] | t^2.04 + 2*t^2.076 + t^2.111 + t^2.834 + t^3.818 + 2*t^3.854 + t^3.889 + t^4.08 + 2*t^4.116 + 4*t^4.151 + 2*t^4.187 + t^4.222 + t^4.874 + 2*t^4.909 + 2*t^4.945 + t^5.667 + t^5.858 + 4*t^5.894 + 5*t^5.929 + 2*t^5.965 - 2*t^6. - t^4.055/y - t^4.055*y | detail |