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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58093 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ | 1.4381 | 1.6248 | 0.8851 | [X:[1.3375], M:[0.9876], q:[0.5645, 0.5521], qb:[0.4355, 0.4603], phi:[0.3313]] | [X:[[6]], M:[[-18]], q:[[13], [-5]], qb:[[-13], [23]], phi:[[-3]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | ${}$ | -2 | 2*t^2.96 + t^2.98 + t^3. + t^3.07 + t^3.96 + t^3.99 + t^4.01 + t^4.03 + t^4.07 + t^4.95 + 2*t^4.99 + t^5.02 + 2*t^5.06 + 2*t^5.93 + 2*t^5.94 + 2*t^5.96 + 2*t^5.98 - 2*t^6. + 2*t^6.04 + 2*t^6.06 + t^6.15 + t^6.9 + t^6.92 + t^6.94 + 2*t^6.96 + 4*t^6.98 + t^6.99 + 2*t^7.01 + 3*t^7.03 + 2*t^7.05 + t^7.07 + t^7.09 + t^7.11 + t^7.12 + t^7.14 + t^7.91 + t^7.93 + 5*t^7.95 + t^7.97 + 3*t^7.99 + t^8.01 + 6*t^8.02 + t^8.04 + 5*t^8.06 + t^8.1 + 3*t^8.14 + 2*t^8.89 + 2*t^8.91 + 2*t^8.93 + 6*t^8.94 - 4*t^8.96 + 2*t^8.98 + t^8.98/y^2 - t^3.99/y - t^4.99/y - (2*t^6.96)/y - t^6.98/y - t^6.99/y - t^7.07/y - (2*t^7.95)/y - t^7.97/y - t^7.99/y - t^8.06/y + t^8.93/y + t^8.94/y + (2*t^8.96)/y - t^3.99*y - t^4.99*y - 2*t^6.96*y - t^6.98*y - t^6.99*y - t^7.07*y - 2*t^7.95*y - t^7.97*y - t^7.99*y - t^8.06*y + t^8.93*y + t^8.94*y + 2*t^8.96*y + t^8.98*y^2 | (2*t^2.96)/g1^18 + t^2.98/g1^9 + t^3. + g1^36*t^3.07 + t^3.96/g1^21 + t^3.99/g1^3 + g1^6*t^4.01 + g1^15*t^4.03 + g1^33*t^4.07 + t^4.95/g1^24 + (2*t^4.99)/g1^6 + g1^12*t^5.02 + 2*g1^30*t^5.06 + (2*t^5.93)/g1^36 + (2*t^5.94)/g1^27 + (2*t^5.96)/g1^18 + (2*t^5.98)/g1^9 - 2*t^6. + 2*g1^18*t^6.04 + 2*g1^27*t^6.06 + g1^72*t^6.15 + t^6.9/g1^48 + t^6.92/g1^39 + t^6.94/g1^30 + (2*t^6.96)/g1^21 + (4*t^6.98)/g1^12 + t^6.99/g1^3 + 2*g1^6*t^7.01 + 3*g1^15*t^7.03 + 2*g1^24*t^7.05 + g1^33*t^7.07 + g1^42*t^7.09 + g1^51*t^7.11 + g1^60*t^7.12 + g1^69*t^7.14 + t^7.91/g1^42 + t^7.93/g1^33 + (5*t^7.95)/g1^24 + t^7.97/g1^15 + (3*t^7.99)/g1^6 + g1^3*t^8.01 + 6*g1^12*t^8.02 + g1^21*t^8.04 + 5*g1^30*t^8.06 + g1^48*t^8.1 + 3*g1^66*t^8.14 + (2*t^8.89)/g1^54 + (2*t^8.91)/g1^45 + (2*t^8.93)/g1^36 + (6*t^8.94)/g1^27 - (4*t^8.96)/g1^18 + (2*t^8.98)/g1^9 + t^8.98/(g1^9*y^2) - t^3.99/(g1^3*y) - t^4.99/(g1^6*y) - (2*t^6.96)/(g1^21*y) - t^6.98/(g1^12*y) - t^6.99/(g1^3*y) - (g1^33*t^7.07)/y - (2*t^7.95)/(g1^24*y) - t^7.97/(g1^15*y) - t^7.99/(g1^6*y) - (g1^30*t^8.06)/y + t^8.93/(g1^36*y) + t^8.94/(g1^27*y) + (2*t^8.96)/(g1^18*y) - (t^3.99*y)/g1^3 - (t^4.99*y)/g1^6 - (2*t^6.96*y)/g1^21 - (t^6.98*y)/g1^12 - (t^6.99*y)/g1^3 - g1^33*t^7.07*y - (2*t^7.95*y)/g1^24 - (t^7.97*y)/g1^15 - (t^7.99*y)/g1^6 - g1^30*t^8.06*y + (t^8.93*y)/g1^36 + (t^8.94*y)/g1^27 + (2*t^8.96*y)/g1^18 + (t^8.98*y^2)/g1^9 |
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 |
---|---|---|---|---|---|---|---|---|---|
57333 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ | 1.4535 | 1.6404 | 0.8861 | [X:[1.3366], M:[0.9901], q:[0.5074, 0.4975], qb:[0.4926, 0.5124], phi:[0.3317]] | 2*t^2.97 + t^2.985 + t^3. + t^3.059 + t^3.965 + t^3.995 + t^4.01 + t^4.025 + t^4.054 + t^4.96 + t^4.99 + t^5.02 + t^5.049 + t^5.488 + t^5.502 + t^5.532 + t^5.547 + 2*t^5.941 + 2*t^5.955 + 2*t^5.97 + t^5.985 - 3*t^6. - t^3.995/y - t^4.99/y - t^3.995*y - t^4.99*y | detail |