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 |
|---|---|---|---|---|---|---|---|---|---|
| 3533 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{4}M_{7}$ | 0.641 | 0.797 | 0.8043 | [X:[1.548], M:[0.452, 1.1827, 0.774, 0.904, 0.8607, 0.7307, 1.096], q:[0.7957, 0.7523], qb:[0.4737, 0.3437], phi:[0.4087]] | [X:[[12]], M:[[-12], [4], [6], [-24], [-14], [16], [24]], q:[[1], [11]], qb:[[-17], [13]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{7}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{5}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{6}M_{7}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{7}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | -2 | t^2.192 + t^2.322 + t^2.452 + t^2.582 + 2*t^3.288 + t^3.548 + t^3.678 + t^4.068 + t^4.384 + 2*t^4.514 + 3*t^4.644 + t^4.774 + 3*t^4.904 + t^5.034 + 2*t^5.48 + t^5.61 + 4*t^5.74 + 3*t^5.87 - 2*t^6. + t^6.13 + t^6.26 - t^6.39 + t^6.52 + 4*t^6.576 + t^6.65 + 2*t^6.706 + 3*t^6.836 + 4*t^6.966 + 3*t^7.096 + t^7.226 + 2*t^7.356 + 2*t^7.486 - t^7.616 + 2*t^7.672 + t^7.746 + 3*t^7.802 + 6*t^7.932 + 2*t^8.062 + t^8.136 + 3*t^8.192 - 3*t^8.452 - 2*t^8.582 + 4*t^8.768 - t^8.842 + 3*t^8.898 + t^8.972 - t^4.226/y - t^6.418/y - t^6.548/y - t^6.808/y + t^7.514/y + (2*t^7.644)/y + (2*t^7.774)/y + (2*t^7.904)/y + (2*t^8.034)/y + (2*t^8.48)/y + t^8.61/y + (2*t^8.74)/y + (3*t^8.87)/y - t^4.226*y - t^6.418*y - t^6.548*y - t^6.808*y + t^7.514*y + 2*t^7.644*y + 2*t^7.774*y + 2*t^7.904*y + 2*t^8.034*y + 2*t^8.48*y + t^8.61*y + 2*t^8.74*y + 3*t^8.87*y | g1^16*t^2.192 + g1^6*t^2.322 + t^2.452/g1^4 + t^2.582/g1^14 + 2*g1^24*t^3.288 + g1^4*t^3.548 + t^3.678/g1^6 + t^4.068/g1^36 + g1^32*t^4.384 + 2*g1^22*t^4.514 + 3*g1^12*t^4.644 + g1^2*t^4.774 + (3*t^4.904)/g1^8 + t^5.034/g1^18 + 2*g1^40*t^5.48 + g1^30*t^5.61 + 4*g1^20*t^5.74 + 3*g1^10*t^5.87 - 2*t^6. + t^6.13/g1^10 + t^6.26/g1^20 - t^6.39/g1^30 + t^6.52/g1^40 + 4*g1^48*t^6.576 + t^6.65/g1^50 + 2*g1^38*t^6.706 + 3*g1^28*t^6.836 + 4*g1^18*t^6.966 + 3*g1^8*t^7.096 + t^7.226/g1^2 + (2*t^7.356)/g1^12 + (2*t^7.486)/g1^22 - t^7.616/g1^32 + 2*g1^56*t^7.672 + t^7.746/g1^42 + 3*g1^46*t^7.802 + 6*g1^36*t^7.932 + 2*g1^26*t^8.062 + t^8.136/g1^72 + 3*g1^16*t^8.192 - (3*t^8.452)/g1^4 - (2*t^8.582)/g1^14 + 4*g1^64*t^8.768 - t^8.842/g1^34 + 3*g1^54*t^8.898 + t^8.972/g1^44 - t^4.226/(g1^2*y) - (g1^14*t^6.418)/y - (g1^4*t^6.548)/y - t^6.808/(g1^16*y) + (g1^22*t^7.514)/y + (2*g1^12*t^7.644)/y + (2*g1^2*t^7.774)/y + (2*t^7.904)/(g1^8*y) + (2*t^8.034)/(g1^18*y) + (2*g1^40*t^8.48)/y + (g1^30*t^8.61)/y + (2*g1^20*t^8.74)/y + (3*g1^10*t^8.87)/y - (t^4.226*y)/g1^2 - g1^14*t^6.418*y - g1^4*t^6.548*y - (t^6.808*y)/g1^16 + g1^22*t^7.514*y + 2*g1^12*t^7.644*y + 2*g1^2*t^7.774*y + (2*t^7.904*y)/g1^8 + (2*t^8.034*y)/g1^18 + 2*g1^40*t^8.48*y + g1^30*t^8.61*y + 2*g1^20*t^8.74*y + 3*g1^10*t^8.87*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 |
|---|
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 |
|---|
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2948 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ | 0.6515 | 0.8136 | 0.8007 | [X:[1.5673], M:[0.4327, 1.1891, 0.7836, 0.8655, 0.8382, 0.7563], q:[0.7973, 0.77], qb:[0.4464, 0.3645], phi:[0.4055]] | t^2.269 + t^2.351 + t^2.433 + t^2.515 + t^2.596 + t^3.404 + t^3.567 + t^3.649 + t^3.895 + t^4.538 + 2*t^4.62 + 3*t^4.702 + t^4.784 + 4*t^4.865 + 2*t^4.947 + t^5.029 + t^5.111 + t^5.193 + t^5.673 + 3*t^5.836 + 2*t^5.918 - t^6. - t^4.216/y - t^4.216*y | detail |