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 |
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48261 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{3}^{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6652 | 0.8849 | 0.7517 | [M:[0.7275, 0.6976, 1.0, 0.7575, 0.7275], q:[0.7575, 0.515], qb:[0.5449, 0.2425], phi:[0.485]] | [M:[[3], [7], [0], [-1], [3]], q:[[-1], [-2]], qb:[[-6], [1]], phi:[[2]]] |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }M_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}^{3}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{2}^{4}$ | ${}$ | -3 | t^2.093 + 2*t^2.183 + 2*t^2.272 + t^2.362 + 2*t^2.91 + t^3. + t^3.18 + t^4.185 + 2*t^4.275 + 5*t^4.365 + 5*t^4.455 + 6*t^4.545 + 3*t^4.635 + 2*t^4.725 + 2*t^5.003 + 4*t^5.093 + 5*t^5.183 + 5*t^5.272 + 3*t^5.362 + 2*t^5.452 + t^5.542 + 3*t^5.82 - 3*t^6. + t^6.278 + t^6.36 + 2*t^6.368 + 5*t^6.458 + 8*t^6.548 + 10*t^6.638 + 11*t^6.728 + 10*t^6.817 + 7*t^6.907 + 4*t^6.997 + 2*t^7.087 + 2*t^7.096 + 4*t^7.185 + 9*t^7.275 + 11*t^7.365 + 13*t^7.455 + 11*t^7.545 + 8*t^7.635 + 6*t^7.725 + 2*t^7.815 + 2*t^7.904 + 3*t^7.913 + 4*t^8.003 - 4*t^8.183 - 8*t^8.272 - 7*t^8.362 + t^8.371 - 2*t^8.452 + 2*t^8.461 + t^8.542 + 5*t^8.551 + 2*t^8.632 + 8*t^8.64 + t^8.722 + 18*t^8.73 + 14*t^8.82 + 11*t^8.91 - t^4.455/y - t^6.548/y - (2*t^6.638)/y - t^6.728/y + (2*t^7.275)/y + (2*t^7.365)/y + (5*t^7.455)/y + (4*t^7.545)/y + (2*t^7.635)/y + (2*t^8.003)/y + (5*t^8.093)/y + (7*t^8.183)/y + (7*t^8.272)/y + (4*t^8.362)/y + (2*t^8.452)/y + t^8.542/y - t^8.64/y - (2*t^8.73)/y - (3*t^8.82)/y - t^4.455*y - t^6.548*y - 2*t^6.638*y - t^6.728*y + 2*t^7.275*y + 2*t^7.365*y + 5*t^7.455*y + 4*t^7.545*y + 2*t^7.635*y + 2*t^8.003*y + 5*t^8.093*y + 7*t^8.183*y + 7*t^8.272*y + 4*t^8.362*y + 2*t^8.452*y + t^8.542*y - t^8.64*y - 2*t^8.73*y - 3*t^8.82*y | g1^7*t^2.093 + 2*g1^3*t^2.183 + (2*t^2.272)/g1 + t^2.362/g1^5 + 2*g1^4*t^2.91 + t^3. + t^3.18/g1^8 + g1^14*t^4.185 + 2*g1^10*t^4.275 + 5*g1^6*t^4.365 + 5*g1^2*t^4.455 + (6*t^4.545)/g1^2 + (3*t^4.635)/g1^6 + (2*t^4.725)/g1^10 + 2*g1^11*t^5.003 + 4*g1^7*t^5.093 + 5*g1^3*t^5.183 + (5*t^5.272)/g1 + (3*t^5.362)/g1^5 + (2*t^5.452)/g1^9 + t^5.542/g1^13 + 3*g1^8*t^5.82 - 3*t^6. + g1^21*t^6.278 + t^6.36/g1^16 + 2*g1^17*t^6.368 + 5*g1^13*t^6.458 + 8*g1^9*t^6.548 + 10*g1^5*t^6.638 + 11*g1*t^6.728 + (10*t^6.817)/g1^3 + (7*t^6.907)/g1^7 + (4*t^6.997)/g1^11 + (2*t^7.087)/g1^15 + 2*g1^18*t^7.096 + 4*g1^14*t^7.185 + 9*g1^10*t^7.275 + 11*g1^6*t^7.365 + 13*g1^2*t^7.455 + (11*t^7.545)/g1^2 + (8*t^7.635)/g1^6 + (6*t^7.725)/g1^10 + (2*t^7.815)/g1^14 + (2*t^7.904)/g1^18 + 3*g1^15*t^7.913 + 4*g1^11*t^8.003 - 4*g1^3*t^8.183 - (8*t^8.272)/g1 - (7*t^8.362)/g1^5 + g1^28*t^8.371 - (2*t^8.452)/g1^9 + 2*g1^24*t^8.461 + t^8.542/g1^13 + 5*g1^20*t^8.551 + (2*t^8.632)/g1^17 + 8*g1^16*t^8.64 + t^8.722/g1^21 + 18*g1^12*t^8.73 + 14*g1^8*t^8.82 + 11*g1^4*t^8.91 - (g1^2*t^4.455)/y - (g1^9*t^6.548)/y - (2*g1^5*t^6.638)/y - (g1*t^6.728)/y + (2*g1^10*t^7.275)/y + (2*g1^6*t^7.365)/y + (5*g1^2*t^7.455)/y + (4*t^7.545)/(g1^2*y) + (2*t^7.635)/(g1^6*y) + (2*g1^11*t^8.003)/y + (5*g1^7*t^8.093)/y + (7*g1^3*t^8.183)/y + (7*t^8.272)/(g1*y) + (4*t^8.362)/(g1^5*y) + (2*t^8.452)/(g1^9*y) + t^8.542/(g1^13*y) - (g1^16*t^8.64)/y - (2*g1^12*t^8.73)/y - (3*g1^8*t^8.82)/y - g1^2*t^4.455*y - g1^9*t^6.548*y - 2*g1^5*t^6.638*y - g1*t^6.728*y + 2*g1^10*t^7.275*y + 2*g1^6*t^7.365*y + 5*g1^2*t^7.455*y + (4*t^7.545*y)/g1^2 + (2*t^7.635*y)/g1^6 + 2*g1^11*t^8.003*y + 5*g1^7*t^8.093*y + 7*g1^3*t^8.183*y + (7*t^8.272*y)/g1 + (4*t^8.362*y)/g1^5 + (2*t^8.452*y)/g1^9 + (t^8.542*y)/g1^13 - g1^16*t^8.64*y - 2*g1^12*t^8.73*y - 3*g1^8*t^8.82*y |
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 |
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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 |
---|---|---|---|---|---|---|---|---|---|
46550 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{3}^{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.6454 | 0.8481 | 0.761 | [M:[0.7302, 0.7038, 1.0, 0.7566], q:[0.7566, 0.5132], qb:[0.5396, 0.2434], phi:[0.4868]] | t^2.111 + t^2.191 + 2*t^2.27 + t^2.349 + 2*t^2.921 + t^3. + t^3.158 + t^3.809 + t^4.223 + t^4.302 + 3*t^4.381 + 3*t^4.46 + 5*t^4.54 + 3*t^4.619 + 2*t^4.698 + 2*t^5.032 + 2*t^5.111 + 4*t^5.191 + 5*t^5.27 + 2*t^5.349 + 2*t^5.428 + t^5.508 + 3*t^5.842 + t^5.921 - 2*t^6. - t^4.46/y - t^4.46*y | detail |