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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57727 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ | 1.3446 | 1.5364 | 0.8752 | [X:[1.3741], M:[0.6871], q:[0.3537, 0.7279], qb:[0.6463, 0.3946], phi:[0.3129]] | [X:[[0, 2]], M:[[0, 1]], q:[[-1, 4], [-1, 6]], qb:[[1, -4], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{6}$ | ${}\phi_{1}^{3}q_{1}^{3}$, ${ }\phi_{1}^{4}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1 | t^2.06 + t^2.24 + t^2.82 + t^3. + t^3.18 + t^3.37 + 4*t^4.12 + 2*t^4.31 + t^4.49 + t^4.88 + 3*t^5.06 + 4*t^5.24 + 2*t^5.43 + t^5.61 + t^5.63 + t^6. + 7*t^6.18 + 9*t^6.37 + 3*t^6.55 + 2*t^6.73 - 2*t^6.76 + t^6.94 + 5*t^7.12 + 9*t^7.31 + 9*t^7.49 + 3*t^7.67 + t^7.86 - t^7.88 - 2*t^8.06 + 13*t^8.24 + 17*t^8.43 + t^8.45 + 13*t^8.61 + 4*t^8.8 - 2*t^8.82 + 2*t^8.98 + t^8.82/y^2 - t^3.94/y - t^4.88/y - t^6./y - t^6.18/y - t^6.76/y - (2*t^6.94)/y - t^7.12/y - t^7.69/y + t^7.88/y - t^8.06/y + t^8.43/y + t^8.61/y + t^8.82/y - t^3.94*y - t^4.88*y - t^6.*y - t^6.18*y - t^6.76*y - 2*t^6.94*y - t^7.12*y - t^7.69*y + t^7.88*y - t^8.06*y + t^8.43*y + t^8.61*y + t^8.82*y + t^8.82*y^2 | g2*t^2.06 + g2^4*t^2.24 + t^2.82/g2^3 + t^3. + g2^3*t^3.18 + g2^6*t^3.37 + 4*g2^2*t^4.12 + 2*g2^5*t^4.31 + g2^8*t^4.49 + t^4.88/g2^2 + 3*g2*t^5.06 + (g1^3*t^5.24)/g2^5 + 2*g2^4*t^5.24 + (g2^13*t^5.24)/g1^3 + 2*g2^7*t^5.43 + g2^10*t^5.61 + t^5.63/g2^6 - t^6. + (g1^3*t^6.)/g2^9 + (g2^9*t^6.)/g1^3 + (g1^3*t^6.18)/g2^6 + 5*g2^3*t^6.18 + (g2^12*t^6.18)/g1^3 + (g1^3*t^6.37)/g2^3 + 7*g2^6*t^6.37 + (g2^15*t^6.37)/g1^3 + 3*g2^9*t^6.55 + 2*g2^12*t^6.73 - (2*t^6.76)/g2^4 + t^6.94/g2 + 5*g2^2*t^7.12 + (g1^3*t^7.31)/g2^4 + 7*g2^5*t^7.31 + (g2^14*t^7.31)/g1^3 + (g1^3*t^7.49)/g2 + 7*g2^8*t^7.49 + (g2^17*t^7.49)/g1^3 + 3*g2^11*t^7.67 + g2^14*t^7.86 - (g1^3*t^7.88)/g2^11 + t^7.88/g2^2 - (g2^7*t^7.88)/g1^3 - 2*g2*t^8.06 + (2*g1^3*t^8.24)/g2^5 + 9*g2^4*t^8.24 + (2*g2^13*t^8.24)/g1^3 + (3*g1^3*t^8.43)/g2^2 + 11*g2^7*t^8.43 + (3*g2^16*t^8.43)/g1^3 + t^8.45/g2^9 + 2*g1^3*g2*t^8.61 + 9*g2^10*t^8.61 + (2*g2^19*t^8.61)/g1^3 + 4*g2^13*t^8.8 - (2*t^8.82)/g2^3 + 2*g2^16*t^8.98 + t^8.82/(g2^3*y^2) - t^3.94/(g2*y) - t^4.88/(g2^2*y) - t^6./y - (g2^3*t^6.18)/y - t^6.76/(g2^4*y) - (2*t^6.94)/(g2*y) - (g2^2*t^7.12)/y - t^7.69/(g2^5*y) + t^7.88/(g2^2*y) - (g2*t^8.06)/y + (g2^7*t^8.43)/y + (g2^10*t^8.61)/y + t^8.82/(g2^3*y) - (t^3.94*y)/g2 - (t^4.88*y)/g2^2 - t^6.*y - g2^3*t^6.18*y - (t^6.76*y)/g2^4 - (2*t^6.94*y)/g2 - g2^2*t^7.12*y - (t^7.69*y)/g2^5 + (t^7.88*y)/g2^2 - g2*t^8.06*y + g2^7*t^8.43*y + g2^10*t^8.61*y + (t^8.82*y)/g2^3 + (t^8.82*y^2)/g2^3 |
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 |
---|---|---|---|---|---|---|---|---|---|
47950 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.3239 | 1.4959 | 0.885 | [X:[1.3746], q:[0.354, 0.7285], qb:[0.646, 0.3952], phi:[0.3127]] | t^2.247 + t^2.814 + t^3. + t^3.186 + t^3.371 + t^3.938 + 3*t^4.124 + t^4.309 + t^4.495 + 2*t^5.062 + 3*t^5.247 + t^5.433 + t^5.619 + t^5.629 + t^6. - t^3.938/y - t^4.876/y - t^3.938*y - t^4.876*y | detail |